astro-ph9910093.xml


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 urfeld


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 field


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
t0 age


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 larger


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 vacuum expectation value


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 a large rather than a small


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 scale parameter


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 a constant value


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
αg constant


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
αg constant


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
αg


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 non-zero


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0


R2(t,α=0,k<0)=-2A/kcS02-kc2t2
S0 background field


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
Ωk(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯M(t)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩM(t0) the current era


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯M(t)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯M(t0)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯M(t)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩΛ(t) negative


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
Ω¯M(t0)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩΛ(t) control


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯Λ(t0) the quantity


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩΛ(t0) the current era


1Ωk(t0)0
Ω¯Λ(t0) the quantity


1Ωk(t0)0
ΩΛ(t0) the same order of magnitude


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩM(t) future


1Ωk(t0)0
Ω¯M(t0)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
Ω¯Λ(t)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩΛ(t0) the standard model


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
ΩM(t0) the current era


1Ωk(t0)0
ΩM(t)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
Ω¯Λ(t)


1Ωk(t0)0
Ω¯M(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
ΩΛ(t0) it


1Ωk(t0)0
Ω¯Λ(t0)


1Ωk(t0)0
Ω¯M(t0)


1Ωk(t0)0
ΩM(t0)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
Ω¯M(t0) era


1Ωk(t0)0
Ω¯Λ(t0) the current era


1Ωk(t0)0
ΩΛ(t)


1Ωk(t0)0
ΩΛ(t0)


1Ωk(t0)0
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
Ωk(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ωk(t0)


Ω¯M(t0)=0 the rather tight
Ω¯M(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0) the current era


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ω¯M(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
Ωk(t0)=0


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)=0


Ω¯M(t0)=0 the rather tight
Ω¯M(t)


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t) negative


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t) control


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0) the current era


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0 the rather tight
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ωk(t0)=0


Ω¯M(t0)=0 the rather tight
ΩM(t) future


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)=0


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)=0


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0) the standard model


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
ΩM(t0)=0


Ω¯M(t0)=0 the rather tight
ΩM(t0) the current era


Ω¯M(t0)=0 the rather tight
ΩM(t)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0) it


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0)


Ω¯M(t0)=0 the rather tight
ΩM(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
Ωk(t0) orders


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
Ωk(t0)=0


Ω¯M(t0)=0 the rather tight
Ω¯Λ(t0) the current era


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


Ω¯M(t0)=0 the rather tight
ΩΛ(t0)


Ω¯M(t0)=0 the rather tight
ΩΛ(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


α parameter
αg constant


α parameter
αg constant


α parameter
αg


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ωk(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t) negative


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t) control


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t) future


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0) orders


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯M(t0) era


ΩΛ(t0)=0.7
Ω¯Λ(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV a large


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV big or small


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 urfeld


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 field


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tkinμν


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tμν


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tμν the associated energy-momentum tensor


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 larger


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV (highest) critical temperature


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 vacuum expectation value


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 a large rather than a small


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 scale parameter


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tμν


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 a constant value


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 non-zero


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
TV


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
Tmax the temperature


Tmax2-kcS02/2A a maximum (negative curvature supported) temperature
S0 background field


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


α=0
αg constant


α=0
αg constant


α=0
αg


R(t)t
t0 age


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ωk(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t) negative


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t) control


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the current era


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t) future


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the standard model


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0) it


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ωk(t0) orders


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
Ω¯Λ(t0) the current era


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


TV a large
Tmax


TV a large
Tmax


TV a large
Tmax


TV a large
Tkinμν


TV a large
Tmax


TV a large
Tμν


TV a large
Tmax


TV a large
Tμν the associated energy-momentum tensor


TV a large
Tmax


TV a large
Tmax


TV a large
Tμν


TV a large
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV a large
Tmax


TV a large
VminGL which


TV a large
Tmax


TV a large
Tmax the temperature


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ωk(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ωk(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0) the current era


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q0


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
t0 age


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0) the quantity


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0) the current era


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0) the quantity


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0) the same order of magnitude


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t) future


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0) the standard model


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q0


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0) the current era


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0) it


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩM(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ωk(t0) orders


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
q(t0)


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯M(t0) era


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
Ω¯Λ(t0) the current era


q(t)=(n/2-1)ΩM(t)-ΩΛ(t)
ΩΛ(t0)


Λ=VminGL vacuum energy density
Geff small, negative


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
LPL-1 inverse Planck length


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
GF Fermi’s


Λ=VminGL vacuum energy density
Geff


Λ=VminGL vacuum energy density
LPL-1


Λ=VminGL vacuum energy density
Geff the cosmological


Λ=VminGL vacuum energy density
Geff a small, negative


Λ=VminGL vacuum energy density
Geff an appropriate


Λ=VminGL vacuum energy density
Geff


t0H(t0)=arctanh[(-q(t0))1/2]/(-q(t0))1/2 universe
q0


t0H(t0)=arctanh[(-q(t0))1/2]/(-q(t0))1/2 universe
q(t) conformal cosmology


t0H(t0)=arctanh[(-q(t0))1/2]/(-q(t0))1/2 universe
q(t)


t0H(t0)=arctanh[(-q(t0))1/2]/(-q(t0))1/2 universe
q0


-cλS04=σTV4
TV a large


-cλS04=σTV4
Tmax


-cλS04=σTV4
S0


-cλS04=σTV4
TV big or small


-cλS04=σTV4
TV


-cλS04=σTV4
S0


-cλS04=σTV4
S0 urfeld


-cλS04=σTV4
S0 field


-cλS04=σTV4
S0


-cλS04=σTV4
S0


-cλS04=σTV4
Tmax


-cλS04=σTV4
Tmax


-cλS04=σTV4
Tkinμν


-cλS04=σTV4
TV


-cλS04=σTV4
Tmax


-cλS04=σTV4
Tμν


-cλS04=σTV4
Tmax


-cλS04=σTV4
TV


-cλS04=σTV4
Tμν the associated energy-momentum tensor


-cλS04=σTV4
S0 larger


-cλS04=σTV4
Tmax


-cλS04=σTV4
TV


-cλS04=σTV4
TV (highest) critical temperature


-cλS04=σTV4
S0 vacuum expectation value


-cλS04=σTV4
Tmax


-cλS04=σTV4
S0


-cλS04=σTV4
S0 a large rather than a small


-cλS04=σTV4
S0 scale parameter


-cλS04=σTV4
Tμν


-cλS04=σTV4
S0 a constant value


-cλS04=σTV4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


-cλS04=σTV4
Tmax


-cλS04=σTV4
TV


-cλS04=σTV4
VminGL which


-cλS04=σTV4
S0 non-zero


-cλS04=σTV4
S0


-cλS04=σTV4
TV


-cλS04=σTV4
S0


-cλS04=σTV4
Tmax


-cλS04=σTV4
TV


-cλS04=σTV4
TV


-cλS04=σTV4
Tmax the temperature


-cλS04=σTV4
S0 background field


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


q(t0)=0
q0


q(t0)=0
q(t) conformal cosmology


q(t0)=0
q(t)


q(t0)=0
q0


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


ρM(t) perfectly normal
ρM(t0)


ρM(t) perfectly normal
ρM(t0)


ρM(t) perfectly normal
t0 age


ρM(t) perfectly normal
ρM(t0)


ρM(t) perfectly normal
ρM(t0) order


ρM(t) perfectly normal
ρM(t0)


ρM(t)=A/R4=σT4 the complete family of solutions
TV a large


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
ρM(t0)


ρM(t)=A/R4=σT4 the complete family of solutions
TV big or small


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
ρM(t0)


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
Tkinμν


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
Tμν


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
Tμν the associated energy-momentum tensor


ρM(t)=A/R4=σT4 the complete family of solutions
t0 age


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
TV (highest) critical temperature


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
ρM(t0)


ρM(t)=A/R4=σT4 the complete family of solutions
Tμν


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
ρM(t0) order


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
ρM(t0)


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
TV


ρM(t)=A/R4=σT4 the complete family of solutions
Tmax the temperature


TVT(t0)
Tmax


TVT(t0)
T(t)


TVT(t0)
Tmax


TVT(t0)
Tmax


TVT(t0)
TmaxT(t0)


TVT(t0)
Tkinμν


TVT(t0)
Tmax


TVT(t0)
Tμν


TVT(t0)
Tmax


TVT(t0)
Tμν the associated energy-momentum tensor


TVT(t0)
Tmax


TVT(t0)
TmaxT(t0)


TVT(t0)
Tmax


TVT(t0)
Tμν


TVT(t0)
TmaxT(t0)


TVT(t0)
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TVT(t0)
Tmax


TVT(t0)
VminGL which


TVT(t0)
Tmax


TVT(t0)
Tmax the temperature


S0
S0


S0
S0 urfeld


S0
S0 field


S0
S0


S0
S0 larger


S0
S0


S0
S0 a large rather than a small


S0
S0 scale parameter


S0
S0 a constant value


S0
S0 non-zero


S0
S0


S0
S0


S0
S0 background field


ρM(t0)
ρM(t) perfectly normal


ρM(t0)
ρM(t)


ρM(t0)
ρM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff small, negative


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ωk(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ωk(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t) negative


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t) control


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)=8πGρM(t)/3c2H2(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0) the current era


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t) future


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
GF Fermi’s


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0) the standard model


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff the cosmological


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩM(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff a small, negative


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0) it


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff an appropriate


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ωk(t0) orders


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Geff


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯M(t0) era


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
Ω¯Λ(t0) the current era


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t0)


ΩM(t0)=8πGρM(t0)/3c2H2(t0)
ΩΛ(t)


Geff small, negative
GF Fermi’s


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


α1/2ct0 the quantity
αg constant


α1/2ct0 the quantity
αg constant


α1/2ct0 the quantity
αg


Ωk(t)
ΩΛ(t)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
Ωk(t0)


Ωk(t)
Ω¯M(t)


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩM(t)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩM(t0) the current era


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯M(t)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯M(t0)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯M(t)


Ωk(t)
ΩM(t)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩΛ(t) negative


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩΛ(t0)


Ωk(t)
Ω¯M(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩΛ(t) control


Ωk(t)
t0 age


Ωk(t)
ΩM(t)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯Λ(t0) the quantity


Ωk(t)
ΩM(t0)


Ωk(t)
ΩΛ(t0) the current era


Ωk(t)
Ω¯Λ(t0) the quantity


Ωk(t)
ΩΛ(t0) the same order of magnitude


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩM(t)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩM(t) future


Ωk(t)
Ω¯M(t0)


Ωk(t)
ΩM(t)


Ωk(t)
ΩM(t0)


Ωk(t)
Ω¯Λ(t)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩΛ(t0) the standard model


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩM(t)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩM(t)


Ωk(t)
ΩM(t0) the current era


Ωk(t)
ΩM(t)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩΛ(t0)


Ωk(t)
Ω¯Λ(t)


Ωk(t)
Ω¯M(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
ΩΛ(t0) it


Ωk(t)
Ω¯Λ(t0)


Ωk(t)
Ω¯M(t0)


Ωk(t)
ΩM(t0)


Ωk(t)
ΩΛ(t0)


Ωk(t)
Ωk(t0) orders


Ωk(t)
ΩΛ(t)


Ωk(t)
Ω¯M(t0) era


Ωk(t)
Ω¯Λ(t0) the current era


Ωk(t)
ΩΛ(t)


Ωk(t)
ΩΛ(t0)


Ωk(t)
ΩΛ(t)


G>0
Geff small, negative


G>0
Geff


G>0
Geff


G>0
Geff


G>0
Geff


G>0
Geff


G>0
Geff


G>0
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G>0
Geff


G>0
Geff


G>0
Geff


G>0
GF Fermi’s


G>0
Geff


G>0
Geff the cosmological


G>0
Geff a small, negative


G>0
Geff an appropriate


G>0
Geff


TmaxTVT(t0)
T(t)


TmaxTVT(t0)
Tkinμν


TmaxTVT(t0)
Tμν


TmaxTVT(t0)
Tμν the associated energy-momentum tensor


TmaxTVT(t0)
Tμν


TmaxTVT(t0)
VminGL which


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
Ωk(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯M(t)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩM(t0) the current era


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯M(t)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯M(t0)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯M(t)


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩΛ(t) negative


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
Ω¯M(t0)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩΛ(t) control


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯Λ(t0) the quantity


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩΛ(t0) the current era


Ωk(t0)
Ω¯Λ(t0) the quantity


Ωk(t0)
ΩΛ(t0) the same order of magnitude


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩM(t) future


Ωk(t0)
Ω¯M(t0)


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
Ω¯Λ(t)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩΛ(t0) the standard model


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩM(t)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩM(t)


Ωk(t0)
ΩM(t0) the current era


Ωk(t0)
ΩM(t)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
Ω¯Λ(t)


Ωk(t0)
Ω¯M(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
ΩΛ(t0) it


Ωk(t0)
Ω¯Λ(t0)


Ωk(t0)
Ω¯M(t0)


Ωk(t0)
ΩM(t0)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩΛ(t)


Ωk(t0)
Ω¯M(t0) era


Ωk(t0)
Ω¯Λ(t0) the current era


Ωk(t0)
ΩΛ(t)


Ωk(t0)
ΩΛ(t0)


Ωk(t0)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ωk(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ωk(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t) negative


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t) control


Ω¯M(t)
t0 age


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the current era


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩΛ(t0) the same order of magnitude


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t) future


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the standard model


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0) it


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ωk(t0) orders


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯M(t0) era


Ω¯M(t)
Ω¯Λ(t0) the current era


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


β=(1-16Aλ/k2c)1/2 parameters
β*


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


TV big or small
Tmax


TV big or small
Tmax


TV big or small
Tmax


TV big or small
Tkinμν


TV big or small
Tmax


TV big or small
Tμν


TV big or small
Tmax


TV big or small
Tμν the associated energy-momentum tensor


TV big or small
Tmax


TV big or small
Tmax


TV big or small
Tμν


TV big or small
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV big or small
Tmax


TV big or small
VminGL which


TV big or small
Tmax


TV big or small
Tmax the temperature


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩΛ(t,α=0,k<0)
t0 age


ΩΛ(t,α=0,k<0)
αg constant


ΩΛ(t,α=0,k<0)
αg constant


ΩΛ(t,α=0,k<0)
αg


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ωk(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ωk(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t) negative


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t) control


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t) future


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ωk(t0) orders


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯M(t0) era


ΩΛ(t0)=ΩM(t0)+1/2 the line
Ω¯Λ(t0) the current era


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 the line
ΩΛ(t)


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


α matter how large
αg constant


α matter how large
αg constant


α matter how large
αg


S0
S0


S0
S0


S0
S0 vacuum expectation value


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


T(t)
TV a large


T(t)
Tmax


T(t)
TV big or small


T(t)
TV


T(t)
Tmax


T(t)
Tmax


T(t)
Tkinμν


T(t)
T(t0) current temperature


T(t)
TV


T(t)
Tmax


T(t)
Tμν


T(t)
Tmax


T(t)
TV


T(t)
Tμν the associated energy-momentum tensor


T(t)
t0 age


T(t)
Tmax


T(t)
TV


T(t)
TV (highest) critical temperature


T(t)
Tmax


T(t)
Tμν


T(t)
T(t0)


T(t)
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T(t)
Tmax


T(t)
TV


T(t)
TV


T(t)
Tmax


T(t)
TV


T(t)
TV


T(t)
Tmax the temperature


S0 urfeld
S0


S0 urfeld
S0


S0 urfeld
S0 vacuum expectation value


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


-S2Rμμ/12
S0


-S2Rμμ/12
S0


-S2Rμμ/12
S0 urfeld


-S2Rμμ/12
S0 field


-S2Rμμ/12
S0


-S2Rμμ/12
S0


-S2Rμμ/12
S0 larger


-S2Rμμ/12
S0 vacuum expectation value


-S2Rμμ/12
S0


-S2Rμμ/12
S0 a large rather than a small


-S2Rμμ/12
S0 scale parameter


-S2Rμμ/12
S0 a constant value


-S2Rμμ/12
S0 non-zero


-S2Rμμ/12
S0


-S2Rμμ/12
S0


-S2Rμμ/12
S0 background field


α>0
αg constant


α>0
αg constant


α>0
αg


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0 urfeld


αc2=-2λS02=-2λS04/S02 the parameter
S0 field


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0 larger


αc2=-2λS02=-2λS04/S02 the parameter
S0 vacuum expectation value


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0 a large rather than a small


αc2=-2λS02=-2λS04/S02 the parameter
S0 scale parameter


αc2=-2λS02=-2λS04/S02 the parameter
S0 a constant value


αc2=-2λS02=-2λS04/S02 the parameter
αg constant


αc2=-2λS02=-2λS04/S02 the parameter
αg constant


αc2=-2λS02=-2λS04/S02 the parameter
αg


αc2=-2λS02=-2λS04/S02 the parameter
-2λS02


αc2=-2λS02=-2λS04/S02 the parameter
S0 non-zero


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0


αc2=-2λS02=-2λS04/S02 the parameter
S0 background field


Geff
GF Fermi’s


α matter how large
αg constant


α matter how large
αg constant


α matter how large
αg


IW
Wμν


IW
Wμν


IW
Wμν __TABLE_2__


S0 field
S0


S0 field
S0


S0 field
S0 vacuum expectation value


ρM(t0)
ρM(t) perfectly normal


ρM(t0)
ρM(t)


ρM(t0)
ρM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


γ*=-drf(r)r2/2
γ0


γ*=-drf(r)r2/2
dL


-S02/12 the quantity
S0


-S02/12 the quantity
S0


-S02/12 the quantity
S0 urfeld


-S02/12 the quantity
S0 field


-S02/12 the quantity
S0


-S02/12 the quantity
S0


-S02/12 the quantity
S0 larger


-S02/12 the quantity
S0 vacuum expectation value


-S02/12 the quantity
S0


-S02/12 the quantity
S0 a large rather than a small


-S02/12 the quantity
S0 scale parameter


-S02/12 the quantity
S0 a constant value


-S02/12 the quantity
S0 non-zero


-S02/12 the quantity
S0


-S02/12 the quantity
S0


-S02/12 the quantity
S0 background field


Ω¯M(t=0) universe
Ω¯Λ(t=0)


Ω¯M(t=0) universe
t0 age


Ω¯M(t=0) universe
ΩM(t=0) initial


Ω¯M(t=0) universe
ΩΛ(t=0) initial


α
αg constant


α
αg constant


α
αg


G constant
Geff small, negative


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G constant
Geff


G constant
Geff


G constant
Geff


G constant
GF Fermi’s


G constant
Geff


G constant
Geff the cosmological


G constant
Geff a small, negative


G constant
Geff an appropriate


G constant
Geff


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ωk(t)


ΩM(t0) the current era
Ωk(t0)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t) negative


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t) control


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0) the quantity


ΩM(t0) the current era
ΩΛ(t0) the current era


ΩM(t0) the current era
Ω¯Λ(t0) the quantity


ΩM(t0) the current era
ΩΛ(t0) the same order of magnitude


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩM(t) future


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t)


ΩM(t0) the current era
ΩΛ(t0) the standard model


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯Λ(t)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0) it


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ωk(t0) orders


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t0) era


ΩM(t0) the current era
Ω¯Λ(t0) the current era


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


S(x) field
S0


S(x) field
S0


S(x) field
S0 urfeld


S(x) field
S0 field


S(x) field
S0


S(x) field
S0


S(x) field
S0 larger


S(x) field
S0 vacuum expectation value


S(x) field
S0


S(x) field
S0 a large rather than a small


S(x) field
S0 scale parameter


S(x) field
S0 a constant value


S(x) field
S0 non-zero


S(x) field
S0


S(x) field
S0


S(x) field
S0 background field


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


Tmax/TV such a choice
T4/TV4


Tmax/TV such a choice
Tkinμν


Tmax/TV such a choice
Tμν


Tmax/TV such a choice
Tμν the associated energy-momentum tensor


Tmax/TV such a choice
Tμν


Tmax/TV such a choice
TV4/T4


Tmax/TV such a choice
VminGL which


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


R(t)et
t0 age


R(t)
t0 age


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


TVT(t0)
Tmax


TVT(t0)
T(t)


TVT(t0)
Tmax


TVT(t0)
Tmax


TVT(t0)
TmaxT(t0)


TVT(t0)
Tkinμν


TVT(t0)
Tmax


TVT(t0)
Tμν


TVT(t0)
Tmax


TVT(t0)
Tμν the associated energy-momentum tensor


TVT(t0)
Tmax


TVT(t0)
TmaxT(t0)


TVT(t0)
Tmax


TVT(t0)
Tμν


TVT(t0)
TmaxT(t0)


TVT(t0)
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TVT(t0)
Tmax


TVT(t0)
VminGL which


TVT(t0)
Tmax


TVT(t0)
Tmax the temperature


ρM(t)=σT4
TV a large


ρM(t)=σT4
Tmax


ρM(t)=σT4
ρM(t0)


ρM(t)=σT4
TV big or small


ρM(t)=σT4
TV


ρM(t)=σT4
ρM(t0)


ρM(t)=σT4
Tmax


ρM(t)=σT4
Tmax


ρM(t)=σT4
Tkinμν


ρM(t)=σT4
TV


ρM(t)=σT4
Tmax


ρM(t)=σT4
Tμν


ρM(t)=σT4
Tmax


ρM(t)=σT4
TV


ρM(t)=σT4
Tμν the associated energy-momentum tensor


ρM(t)=σT4
t0 age


ρM(t)=σT4
Tmax


ρM(t)=σT4
TV


ρM(t)=σT4
TV (highest) critical temperature


ρM(t)=σT4
Tmax


ρM(t)=σT4
ρM(t0)


ρM(t)=σT4
Tμν


ρM(t)=σT4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


ρM(t)=σT4
Tmax


ρM(t)=σT4
ρM(t0) order


ρM(t)=σT4
TV


ρM(t)=σT4
ρM(t0)


ρM(t)=σT4
TV


ρM(t)=σT4
Tmax


ρM(t)=σT4
TV


ρM(t)=σT4
TV


ρM(t)=σT4
Tmax the temperature


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)=8πGρM(t0)/3c2H2(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ωk(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ωk(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0) the current era


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t) negative


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t) control


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
t0 age


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)=8πGρM(t)/3c2H2(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0) the quantity


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0) the current era


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0) the quantity


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0) the same order of magnitude


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t) future


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
GF Fermi’s


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0) the standard model


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0) the current era


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0) it


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩM(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ωk(t0) orders


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯M(t0) era


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
Ω¯Λ(t0) the current era


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t0)


Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective
ΩΛ(t)


-g00(r)=1-2β*/r+γ*r where and
γ0


S0
S0


S0
S0


S0
S0 vacuum expectation value


Geff
GF Fermi’s


ΩM(t=0)+ΩΛ(t=0)
t0 age


α>0
αg constant


α>0
αg constant


α>0
αg


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


D=8πGΛ/3c
Geff small, negative


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff


D=8πGΛ/3c
GF Fermi’s


D=8πGΛ/3c
Geff


D=8πGΛ/3c
Geff the cosmological


D=8πGΛ/3c
Geff a small, negative


D=8πGΛ/3c
Geff an appropriate


D=8πGΛ/3c
Geff


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ωk(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ωk(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t) negative


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t) control


Ω¯M(t)
t0 age


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the current era


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩΛ(t0) the same order of magnitude


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t) future


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the standard model


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0) it


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ωk(t0) orders


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯M(t0) era


Ω¯M(t)
Ω¯Λ(t0) the current era


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


10-60 order
10-2 order


10-60 order
1060 order


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ωk(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ωk(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯M(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 urfeld


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 field


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0) the current era


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
LPL-1 inverse Planck length


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯M(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯M(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t) negative


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t) control


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 larger


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0) the quantity


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 vacuum expectation value


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0) the current era


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0) the quantity


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t) future


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 a large rather than a small


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 scale parameter


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
LPL-1


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 a constant value


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0) the standard model


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0) the current era


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 non-zero


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0) it


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩM(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ωk(t0) orders


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
S0 background field


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
Ω¯Λ(t0) the current era


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t0)


Ω¯M(t0)=-3ΩM(t0)/4πS02LPL2 it
ΩΛ(t)


Geff
GF Fermi’s


q(t,α>0,k<0)
q0


q(t,α>0,k<0)
t0 age


q(t,α>0,k<0)
αg constant


q(t,α>0,k<0)
αg constant


q(t,α>0,k<0)
q0


q(t,α>0,k<0)
αg


S0
S0


S0
S0 urfeld


S0
S0 field


S0
S0


S0
S0 larger


S0
S0


S0
S0 a large rather than a small


S0
S0 scale parameter


S0
S0 a constant value


S0
S0 non-zero


S0
S0


S0
S0


S0
S0 background field


dL=cH(t0)-1(z+z2)
LPL-1 inverse Planck length


dL=cH(t0)-1(z+z2)
LPL-1


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV a large


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff small, negative


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV big or small


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
LPL-1 inverse Planck length


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tkinμν


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tμν


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tμν the associated energy-momentum tensor


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV (highest) critical temperature


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
GF Fermi’s


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tμν


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
LPL-1


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff the cosmological


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff a small, negative


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff an appropriate


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
TV


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Geff


VminGL=-g(TV2-T2)2 necessarily negative vacuum energy density
Tmax the temperature


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


T<TV
Tmax


T<TV
Tmax


T<TV
Tmax


T<TV
Tkinμν


T<TV
Tmax


T<TV
Tμν


T<TV
Tmax


T<TV
Tμν the associated energy-momentum tensor


T<TV
Tmax


T<TV
Tmax


T<TV
Tμν


T<TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T<TV
Tmax


T<TV
VminGL which


T<TV
Tmax


T<TV
Tmax the temperature


R2(t,α=0,k<0) Eq
t0 age


R2(t,α=0,k<0) Eq
αg constant


R2(t,α=0,k<0) Eq
αg constant


R2(t,α=0,k<0) Eq
αg


D=8π(-G)(-Λ)/3c
Geff small, negative


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
GF Fermi’s


D=8π(-G)(-Λ)/3c
Geff


D=8π(-G)(-Λ)/3c
Geff the cosmological


D=8π(-G)(-Λ)/3c
Geff a small, negative


D=8π(-G)(-Λ)/3c
Geff an appropriate


D=8π(-G)(-Λ)/3c
Geff


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ωk(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ωk(t0)


ΩΛ(t0)=1
Ω¯M(t)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
ΩM(t0) the current era


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯M(t)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯M(t0)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯M(t)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩΛ(t) negative


ΩΛ(t0)=1
Ω¯M(t0)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩΛ(t) control


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯Λ(t0) the quantity


ΩΛ(t0)=1
Ωk(t0)=1


ΩΛ(t0)=1
Ωk(t0)=1


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯Λ(t0) the quantity


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩM(t) future


ΩΛ(t0)=1
Ω¯M(t0)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ω¯Λ(t)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩM(t0)=1


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
ΩM(t0) the current era


ΩΛ(t0)=1
ΩM(t)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
Ω¯Λ(t)


ΩΛ(t0)=1
Ω¯M(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ω¯Λ(t0)


ΩΛ(t0)=1
Ω¯M(t0)


ΩΛ(t0)=1
ΩM(t0)


ΩΛ(t0)=1
Ωk(t0) orders


ΩΛ(t0)=1
Ωk(t0)=1


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
Ω¯M(t0) era


ΩΛ(t0)=1
Ω¯Λ(t0) the current era


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t0)=1
ΩΛ(t)


ΩΛ(t=,α>0)
t0 age


ΩΛ(t=,α>0)
αg constant


ΩΛ(t=,α>0)
αg constant


ΩΛ(t=,α>0)
αg


-1060 order
10-60 order


-1060 order
10-2 order


-1060 order
-10120


ΩM(t=0)+ΩΛ(t=0)=1
t0 age


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ωk(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ωk(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t) negative


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t) control


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the current era


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t) future


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the standard model


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0) it


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ωk(t0) orders


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0) the current era


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


T(t)Tmax all times
TV a large


T(t)Tmax all times
TV big or small


T(t)Tmax all times
TV


T(t)Tmax all times
Tkinμν


T(t)Tmax all times
T(t0) current temperature


T(t)Tmax all times
TV


T(t)Tmax all times
Tμν


T(t)Tmax all times
TV


T(t)Tmax all times
Tμν the associated energy-momentum tensor


T(t)Tmax all times
t0 age


T(t)Tmax all times
TV


T(t)Tmax all times
TV (highest) critical temperature


T(t)Tmax all times
Tμν


T(t)Tmax all times
T(t0)


T(t)Tmax all times
TV


T(t)Tmax all times
TV


T(t)Tmax all times
TV


T(t)Tmax all times
TV


q(t)0
q(t0)


q(t)0
q0


q(t)0
q(t0)


q(t)0
q(t0)


q(t)0
t0 age


q(t)0
q0


q(t)0
q(t0)


q(t)0
q(t0)


q(t)0
q(t0)


G effective
Geff small, negative


G effective
Geff


G effective
Geff


G effective
Geff


G effective
Geff


G effective
Geff


G effective
Geff


G effective
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G effective
Geff


G effective
Geff


G effective
Geff


G effective
GF Fermi’s


G effective
Geff


G effective
Geff the cosmological


G effective
Geff a small, negative


G effective
Geff an appropriate


G effective
Geff


Geff
GF Fermi’s


α>0
αg constant


α>0
αg constant


α>0
αg


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


sech2(α1/2ct0)
αg constant


sech2(α1/2ct0)
αg constant


sech2(α1/2ct0)
αg


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


Ωk(t0)=0
Ω¯M(t0)=0 the rather tight


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ωk(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t) negative


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t) control


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the current era


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩΛ(t0) the same order of magnitude


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t) future


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the standard model


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0 viz.


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0) it


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯M(t0) era


Ωk(t0)=0
Ω¯Λ(t0) the current era


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0 urfeld


Geff=-3c3/4πS02
S0 field


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0 larger


Geff=-3c3/4πS02
S0 vacuum expectation value


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0 a large rather than a small


Geff=-3c3/4πS02
S0 scale parameter


Geff=-3c3/4πS02
GF Fermi’s


Geff=-3c3/4πS02
S0 a constant value


Geff=-3c3/4πS02
S0 non-zero


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0


Geff=-3c3/4πS02
S0 background field


Geff
GF Fermi’s


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


TV1016K
Tmax


TV1016K
10-60 order


TV1016K
Tmax


TV1016K
Tmax


TV1016K
Tkinμν


TV1016K
Tmax


TV1016K
Tμν


TV1016K
Tmax


TV1016K
Tμν the associated energy-momentum tensor


TV1016K
Tmax


TV1016K
Tmax


TV1016K
Tμν


TV1016K
10-2 order


TV1016K
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV1016K
Tmax


TV1016K
VminGL which


TV1016K
1060 order


TV1016K
Tmax


TV1016K
Tmax the temperature


tanh2(α1/2ct0)
tanh(α1/2ct0)


tanh2(α1/2ct0)
αg constant


tanh2(α1/2ct0)
αg constant


tanh2(α1/2ct0)
αg


T4/TV4
TV a large


T4/TV4
Tmax


T4/TV4
TV big or small


T4/TV4
TV


T4/TV4
Tmax/TV such a choice


T4/TV4
Tmax


T4/TV4
Tmax


T4/TV4
Tkinμν


T4/TV4
TV


T4/TV4
Tmax


T4/TV4
Tμν


T4/TV4
Tmax


T4/TV4
TV


T4/TV4
Tμν the associated energy-momentum tensor


T4/TV4
Tmax


T4/TV4
TV


T4/TV4
TV (highest) critical temperature


T4/TV4
Tmax


T4/TV4
Tμν


T4/TV4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T4/TV4
Tmax


T4/TV4
TV4/T4


T4/TV4
TV


T4/TV4
VminGL which


T4/TV4
TV


T4/TV4
Tmax


T4/TV4
TV


T4/TV4
TV


T4/TV4
Tmax the temperature


R˙(t)/R(t)=α1/2c
R(t)


R˙(t)/R(t)=α1/2c
R(t)


R˙(t)/R(t)=α1/2c
t0 age


R˙(t)/R(t)=α1/2c
αc2


R˙(t)/R(t)=α1/2c
αg constant


R˙(t)/R(t)=α1/2c
αg constant


R˙(t)/R(t)=α1/2c
αg


R˙(t)/R(t)=α1/2c
R(t)


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


α>0, k=0
αg constant


α>0, k=0
αg constant


α>0, k=0
αg


α>0
αg constant


α>0
αg constant


α>0
αg


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ωk(t)


ΩM(t0)=0.3
Ωk(t0)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t) negative


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t) control


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the current era


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the same order of magnitude


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t) future


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
ΩΛ(t0) the standard model


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0) it


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ωk(t0) orders


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0) era


ΩM(t0)=0.3
Ω¯Λ(t0) the current era


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


ΩΛ(t0)=0
Ω¯M(t0)=0 the rather tight


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ωk(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t0) the current era


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t) negative


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩΛ(t) control


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
ΩM(t) future


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t)


ΩΛ(t0)=0
ΩM(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)=0


ΩΛ(t0)=0
ΩM(t0) the current era


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ω¯M(t0)=0 viz.


ΩΛ(t0)=0
Ω¯Λ(t)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0) orders


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
Ω¯M(t0) era


ΩΛ(t0)=0
Ω¯Λ(t0) the current era


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t)


TmaxT(t0)
TV a large


TmaxT(t0)
TVT(t0)


TmaxT(t0)
TV big or small


TmaxT(t0)
TV


TmaxT(t0)
T(t)


TmaxT(t0)
TVT(t0)


TmaxT(t0)
Tkinμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν the associated energy-momentum tensor


TmaxT(t0)
TV


TmaxT(t0)
TV (highest) critical temperature


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ωk(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ωk(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t) negative


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t) control


Ω¯M(t)
t0 age


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the current era


Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯M(t)
ΩΛ(t0) the same order of magnitude


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩM(t) future


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0) the standard model


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩM(t)


Ω¯M(t)
ΩM(t0) the current era


Ω¯M(t)
ΩM(t)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ω¯Λ(t)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
ΩΛ(t0) it


Ω¯M(t)
Ω¯Λ(t0)


Ω¯M(t)
Ω¯M(t0)


Ω¯M(t)
ΩM(t0)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
Ωk(t0) orders


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
Ω¯M(t0) era


Ω¯M(t)
Ω¯Λ(t0) the current era


Ω¯M(t)
ΩΛ(t)


Ω¯M(t)
ΩΛ(t0)


Ω¯M(t)
ΩΛ(t)


Tkinμν
TV a large


Tkinμν
Tmax


Tkinμν
TV big or small


Tkinμν
TV


Tkinμν
Tmax


Tkinμν
Tmax


Tkinμν
TV


Tkinμν
Tmax


Tkinμν
Tμν


Tkinμν
Tmax


Tkinμν
TV


Tkinμν
Tμν the associated energy-momentum tensor


Tkinμν
Tmax


Tkinμν
TV


Tkinμν
TV (highest) critical temperature


Tkinμν
Tmax


Tkinμν
Tμν


Tkinμν
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tkinμν
Tmax


Tkinμν
TV


Tkinμν
TV


Tkinμν
Tmax


Tkinμν
TV


Tkinμν
TV


Tkinμν
Tmax the temperature


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ωk(t)


ΩM(t0)ΩΛ(t0)
Ωk(t0)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t) negative


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t) control


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩM(t) future


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
Ωk(t0) orders


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0) era


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩΛ(t,α>0,k>0) the positive spatial 3-curvature
t0 age


ΩΛ(t,α>0,k>0) the positive spatial 3-curvature
αg constant


ΩΛ(t,α>0,k>0) the positive spatial 3-curvature
αg constant


ΩΛ(t,α>0,k>0) the positive spatial 3-curvature
αg


α>0
αg constant


α>0
αg constant


α>0
αg


α>0
αg constant


α>0
αg constant


α>0
αg


Λ=λS04
S0


Λ=λS04
S0


Λ=λS04
S0 urfeld


Λ=λS04
S0 field


Λ=λS04
S0


Λ=λS04
S0


Λ=λS04
S0 larger


Λ=λS04
S0 vacuum expectation value


Λ=λS04
S0


Λ=λS04
S0 a large rather than a small


Λ=λS04
S0 scale parameter


Λ=λS04
S0 a constant value


Λ=λS04
S0 non-zero


Λ=λS04
S0


Λ=λS04
S0


Λ=λS04
S0 background field


Ω¯Λ(t=0)
Ω¯M(t=0) universe


Ω¯Λ(t=0)
t0 age


Ω¯Λ(t=0)
Ω¯M(t=0)


Ω¯Λ(t=0)
ΩM(t=0) initial


Ω¯Λ(t=0)
ΩΛ(t=0) initial


α the parameter
αg constant


α the parameter
αg constant


α the parameter
αg


α>0
αg constant


α>0
αg constant


α>0
αg


q(t)-
q(t0)


q(t)-
q0


q(t)-
q(t0)


q(t)-
q(t0)


q(t)-
t0 age


q(t)-
q0


q(t)-
q(t0)


q(t)-
q(t0)


q(t)-
q(t0)


α>0
αg constant


α>0
αg constant


α>0
αg


T(t0) current temperature
TV a large


T(t0) current temperature
Tmax


T(t0) current temperature
TV big or small


T(t0) current temperature
TV


T(t0) current temperature
T(t)


T(t0) current temperature
Tmax


T(t0) current temperature
Tmax


T(t0) current temperature
Tkinμν


T(t0) current temperature
TV


T(t0) current temperature
Tmax


T(t0) current temperature
Tμν


T(t0) current temperature
Tmax


T(t0) current temperature
TV


T(t0) current temperature
Tμν the associated energy-momentum tensor


T(t0) current temperature
Tmax


T(t0) current temperature
TV


T(t0) current temperature
TV (highest) critical temperature


T(t0) current temperature
Tmax


T(t0) current temperature
Tμν


T(t0) current temperature
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T(t0) current temperature
Tmax


T(t0) current temperature
TV


T(t0) current temperature
TV


T(t0) current temperature
Tmax


T(t0) current temperature
TV


T(t0) current temperature
TV


T(t0) current temperature
Tmax the temperature


Geff
GF Fermi’s


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ωk(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ωk(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0) the current era


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t) negative


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t) control


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
tanh(α1/2ct0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0) the current era


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t) future


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯Λ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)=tanh2(α1/2ct0)
αg constant


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
αg constant


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
αg


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0) the current era


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯Λ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0) it


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩM(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ωk(t0) orders


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
Ω¯M(t0) era


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t0)


Ω¯Λ(t0)=tanh2(α1/2ct0)
ΩΛ(t)


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem
GF Fermi’s


S(x)=0
S0


S(x)=0
S0


S(x)=0
S0 urfeld


S(x)=0
S0 field


S(x)=0
S0


S(x)=0
S0


S(x)=0
S0 larger


S(x)=0
S0 vacuum expectation value


S(x)=0
S0


S(x)=0
S0 a large rather than a small


S(x)=0
S0 scale parameter


S(x)=0
S0 a constant value


S(x)=0
S0 non-zero


S(x)=0
S0


S(x)=0
S0


S(x)=0
S0 background field


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


t=0
t0 age


t=dτ/R(τ)
t0 age


t=dτ/R(τ)
dL


c|Λ|=σTV4
TV a large


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
TV big or small


c|Λ|=σTV4
TV


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
Tkinμν


c|Λ|=σTV4
TV


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
Tμν


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
TV


c|Λ|=σTV4
Tμν the associated energy-momentum tensor


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
TV


c|Λ|=σTV4
TV (highest) critical temperature


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
Tμν


c|Λ|=σTV4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
TV


c|Λ|=σTV4
VminGL which


c|Λ|=σTV4
TV


c|Λ|=σTV4
Tmax


c|Λ|=σTV4
TV


c|Λ|=σTV4
TV


c|Λ|=σTV4
Tmax the temperature


R˙(t=0)
t0 age


α=8πGeffΛ/3c3
GF Fermi’s


α=8πGeffΛ/3c3
αg constant


α=8πGeffΛ/3c3
αg constant


α=8πGeffΛ/3c3
αg


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ωk(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ωk(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0) the current era


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
t0 age


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0) the current era


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t) future


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0) the standard model


ΩΛ(t)=αc2R2(t)/R˙2(t)
αg constant


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
αg constant


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
αg


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0) the current era


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0) it


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩM(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ωk(t0) orders


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯M(t0) era


ΩΛ(t)=αc2R2(t)/R˙2(t)
Ω¯Λ(t0) the current era


ΩΛ(t)=αc2R2(t)/R˙2(t)
ΩΛ(t0)


S(x)
S0


S(x)
S0


S(x)
S0 urfeld


S(x)
S0 field


S(x)
S0


S(x)
S0


S(x)
S0 larger


S(x)
S0 vacuum expectation value


S(x)
S0


S(x)
S0 a large rather than a small


S(x)
S0 scale parameter


S(x)
S0 a constant value


S(x)
S0 non-zero


S(x)
S0


S(x)
S0


S(x)
S0 background field


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t) negative


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t) control


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
t0 age


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)=8πGΛ/3cH2(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t) future


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
GF Fermi’s


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the standard model


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) it


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t0) orders


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0) era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


ρM(t)=B/R3
ρM(t0)


ρM(t)=B/R3
ρM(t0)


ρM(t)=B/R3
t0 age


ρM(t)=B/R3
ρM(t0)


ρM(t)=B/R3
ρM(t0) order


ρM(t)=B/R3
ρM(t0)


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
Ωk(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ωk(t0)


ΩΛ(t) negative
Ω¯M(t)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩM(t0) the current era


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯M(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯M(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯M(t)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
Ω¯M(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
t0 age


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯Λ(t0) the quantity


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩΛ(t0) the current era


ΩΛ(t) negative
Ω¯Λ(t0) the quantity


ΩΛ(t) negative
ΩΛ(t0) the same order of magnitude


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩM(t) future


ΩΛ(t) negative
Ω¯M(t0)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
Ω¯Λ(t)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩΛ(t0) the standard model


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
ΩM(t0) the current era


ΩΛ(t) negative
ΩM(t)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
Ω¯Λ(t)


ΩΛ(t) negative
Ω¯M(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
ΩΛ(t0) it


ΩΛ(t) negative
Ω¯Λ(t0)


ΩΛ(t) negative
Ω¯M(t0)


ΩΛ(t) negative
ΩM(t0)


ΩΛ(t) negative
ΩΛ(t0)


ΩΛ(t) negative
Ωk(t0) orders


ΩΛ(t) negative
Ω¯M(t0) era


ΩΛ(t) negative
Ω¯Λ(t0) the current era


ΩΛ(t) negative
ΩΛ(t0)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


S(x) field
S0


S(x) field
S0


S(x) field
S0 urfeld


S(x) field
S0 field


S(x) field
S0


S(x) field
S0


S(x) field
S0 larger


S(x) field
S0 vacuum expectation value


S(x) field
S0


S(x) field
S0 a large rather than a small


S(x) field
S0 scale parameter


S(x) field
S0 a constant value


S(x) field
S0 non-zero


S(x) field
S0


S(x) field
S0


S(x) field
S0 background field


R(t)
t0 age


Tμν
TV a large


Tμν
Tmax


Tμν
TV big or small


Tμν
TV


Tμν
Tmax


Tμν
Tmax


Tμν
Tkinμν


Tμν
TV


Tμν
Tmax


Tμν
Tmax


Tμν
TV


Tμν
Tmax


Tμν
TV


Tμν
TV (highest) critical temperature


Tμν
Tmax


Tμν
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tμν
Tmax


Tμν
TV


Tμν
TV


Tμν
Tmax


Tμν
TV


Tμν
TV


Tμν
Tmax the temperature


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ωk(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t) negative


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t) control


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the current era


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t) future


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the standard model


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0) it


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ωk(t0) orders


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
Ω¯Λ(t0) the current era


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


q(t0)=-1 the deceleration parameter
q0


q(t0)=-1 the deceleration parameter
q(t) conformal cosmology


q(t0)=-1 the deceleration parameter
q(t)


q(t0)=-1 the deceleration parameter
q0


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ωk(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ωk(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t) negative


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t) control


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the current era


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t) future


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the standard model


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0) it


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ωk(t0) orders


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0) the current era


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


Tμν the associated energy-momentum tensor
TV a large


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
TV big or small


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
Tkinμν


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
TV (highest) critical temperature


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
Tmax


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
TV


Tμν the associated energy-momentum tensor
Tmax the temperature


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
Ωk(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ωk(t0)


ΩΛ(t) control
Ω¯M(t)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩM(t0) the current era


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯M(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯M(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯M(t)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
Ω¯M(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
t0 age


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯Λ(t0) the quantity


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩΛ(t0) the current era


ΩΛ(t) control
Ω¯Λ(t0) the quantity


ΩΛ(t) control
ΩΛ(t0) the same order of magnitude


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩM(t) future


ΩΛ(t) control
Ω¯M(t0)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
Ω¯Λ(t)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩΛ(t0) the standard model


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
ΩM(t0) the current era


ΩΛ(t) control
ΩM(t)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
Ω¯Λ(t)


ΩΛ(t) control
Ω¯M(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
ΩΛ(t0) it


ΩΛ(t) control
Ω¯Λ(t0)


ΩΛ(t) control
Ω¯M(t0)


ΩΛ(t) control
ΩM(t0)


ΩΛ(t) control
ΩΛ(t0)


ΩΛ(t) control
Ωk(t0) orders


ΩΛ(t) control
Ω¯M(t0) era


ΩΛ(t) control
Ω¯Λ(t0) the current era


ΩΛ(t) control
ΩΛ(t0)


ρM(t)=A/Rn(t)
ρM(t0)


ρM(t)=A/Rn(t)
ρM(t0)


ρM(t)=A/Rn(t)
t0 age


ρM(t)=A/Rn(t)
ρM(t0)


ρM(t)=A/Rn(t)
ρM(t0) order


ρM(t)=A/Rn(t)
ρM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ωk(t)


ΩM(t0)=0.3
Ωk(t0)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t) negative


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t) control


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the current era


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the same order of magnitude


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t) future


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
ΩΛ(t0) the standard model


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0) it


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ωk(t0) orders


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0) era


ΩM(t0)=0.3
Ω¯Λ(t0) the current era


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
Ωk(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ωk(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0) the current era


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t) negative


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t) control


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) the current era


0Ω¯Λ(t0)1
ΩΛ(t0) the same order of magnitude


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t) future


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯Λ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) the standard model


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0) the current era


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ω¯Λ(t)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) it


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ωk(t0) orders


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
Ω¯M(t0) era


0Ω¯Λ(t0)1
0ΩΛ(t)1


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ωk(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0) the current era


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t) negative


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t) control


Ωk(t)=-kc2/R˙2(t)
t0 age


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0) the quantity


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0) the current era


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0) the quantity


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0) the same order of magnitude


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t) future


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0) the standard model


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0) the current era


Ωk(t)=-kc2/R˙2(t)
ΩM(t)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0) it


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0)


Ωk(t)=-kc2/R˙2(t)
ΩM(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
Ωk(t0) orders


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
Ω¯M(t0) era


Ωk(t)=-kc2/R˙2(t)
Ω¯Λ(t0) the current era


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t0)


Ωk(t)=-kc2/R˙2(t)
ΩΛ(t)


S0 larger
S0


S0 larger
S0


S0 larger
S0 vacuum expectation value


Geff
GF Fermi’s


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ωk(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ωk(t0)


ΩΛ(t0)0.7
Ω¯M(t)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
ΩM(t0) the current era


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯M(t)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯M(t0)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯M(t)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩΛ(t) negative


ΩΛ(t0)0.7
Ω¯M(t0)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩΛ(t) control


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩM(t) future


ΩΛ(t0)0.7
Ω¯M(t0)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ω¯Λ(t)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
ΩM(t0) the current era


ΩΛ(t0)0.7
ΩM(t)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
Ω¯Λ(t)


ΩΛ(t0)0.7
Ω¯M(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ω¯Λ(t0)


ΩΛ(t0)0.7
Ω¯M(t0)


ΩΛ(t0)0.7
ΩM(t0)


ΩΛ(t0)0.7
Ωk(t0) orders


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
Ω¯M(t0) era


ΩΛ(t0)0.7
Ω¯Λ(t0) the current era


ΩΛ(t0)0.7
ΩΛ(t)


ΩΛ(t0)0.7
ΩΛ(t)


tanh(α1/2ct0)
tanh2(α1/2ct0)


tanh(α1/2ct0)
αg constant


tanh(α1/2ct0)
αg constant


tanh(α1/2ct0)
αg


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ωk(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
Ω¯M(t)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t) negative


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t) control


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the current era


Ω¯M(t0)=0
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
ΩM(t) future


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩΛ(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0) the standard model


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
ΩM(t0)=0


Ω¯M(t0)=0
ΩM(t0) the current era


Ω¯M(t0)=0
ΩM(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ω¯Λ(t)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩΛ(t0) it


Ω¯M(t0)=0
Ω¯Λ(t0)


Ω¯M(t0)=0
ΩM(t0)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
Ωk(t0) orders


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
Ωk(t0)=0


Ω¯M(t0)=0
Ω¯Λ(t0) the current era


Ω¯M(t0)=0
ΩΛ(t)


Ω¯M(t0)=0
ΩΛ(t0)


Ω¯M(t0)=0
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)=8πGρM(t0)/3c2H2(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff small, negative


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ωk(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ωk(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0) the current era


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t)=8πGeffρM(t)/3c2H2(t) effective


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t) negative


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t) control


ΩM(t)=8πGρM(t)/3c2H2(t)
t0 age


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0) the quantity


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0) the current era


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0) the quantity


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
GF Fermi’s


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0) the standard model


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff the cosmological


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0) the current era


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff a small, negative


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0) it


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩM(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff an appropriate


ΩM(t)=8πGρM(t)/3c2H2(t)
Ωk(t0) orders


ΩM(t)=8πGρM(t)/3c2H2(t)
Geff


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯M(t0) era


ΩM(t)=8πGρM(t)/3c2H2(t)
Ω¯Λ(t0) the current era


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t0)


ΩM(t)=8πGρM(t)/3c2H2(t)
ΩΛ(t)


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


α
αg constant


α
αg constant


α
αg


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
Ωk(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ωk(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0) the current era


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t) negative


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t) control


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) the current era


Ω¯Λ(t0) the quantity
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t) future


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯Λ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) the standard model


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0) the current era


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ω¯Λ(t)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) it


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ωk(t0) orders


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
Ω¯M(t0) era


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


q(t) conformal cosmology
q(t0)


q(t) conformal cosmology
q0


q(t) conformal cosmology
q(t0)


q(t) conformal cosmology
q(t0)


q(t) conformal cosmology
t0 age


q(t) conformal cosmology
q0


q(t) conformal cosmology
q(t0)


q(t) conformal cosmology
q(t0)


q(t) conformal cosmology
q(t0)


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ωk(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)=1


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t) negative


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t) control


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the current era


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩΛ(t0) the same order of magnitude


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t) future


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the standard model


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)=1


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0) it


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯M(t0) era


Ωk(t0)=1
Ω¯Λ(t0) the current era


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tkinμν


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tμν


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tμν the associated energy-momentum tensor


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tμν


TV (highest) critical temperature
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
VminGL which


TV (highest) critical temperature
Tmax


TV (highest) critical temperature
Tmax the temperature


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ωk(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)=1


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t) negative


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t) control


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the current era


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩΛ(t0) the same order of magnitude


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t) future


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the standard model


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)=1


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0) it


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯M(t0) era


Ωk(t0)=1
Ω¯Λ(t0) the current era


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff small, negative


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ωk(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ωk(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0) the current era


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t)=8πGeffΛ/3cH2(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
t0 age


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0) the current era


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t)=8πGeffΛ/3cH2(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t) future


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
GF Fermi’s


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0) the standard model


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff the cosmological


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0) the current era


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff a small, negative


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0) it


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩM(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


ΩΛ(t)=8πGΛ/3cH2(t)
Geff an appropriate


ΩΛ(t)=8πGΛ/3cH2(t)
Ωk(t0) orders


ΩΛ(t)=8πGΛ/3cH2(t)
Geff


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯M(t0) era


ΩΛ(t)=8πGΛ/3cH2(t)
Ω¯Λ(t0) the current era


ΩΛ(t)=8πGΛ/3cH2(t)
ΩΛ(t0)


dL=cH(t0)-1(z+z2/2)
LPL-1 inverse Planck length


dL=cH(t0)-1(z+z2/2)
LPL-1


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


TmaxT(t0)
TV a large


TmaxT(t0)
TVT(t0)


TmaxT(t0)
TV big or small


TmaxT(t0)
TV


TmaxT(t0)
T(t)


TmaxT(t0)
TVT(t0)


TmaxT(t0)
Tkinμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν the associated energy-momentum tensor


TmaxT(t0)
TV


TmaxT(t0)
TV (highest) critical temperature


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


S0 vacuum expectation value
S0


S0 vacuum expectation value
S0 urfeld


S0 vacuum expectation value
S0 field


S0 vacuum expectation value
S0


S0 vacuum expectation value
S0 larger


S0 vacuum expectation value
S0


S0 vacuum expectation value
S0 a large rather than a small


S0 vacuum expectation value
S0 scale parameter


S0 vacuum expectation value
S0 a constant value


S0 vacuum expectation value
S0 non-zero


S0 vacuum expectation value
S0


S0 vacuum expectation value
S0


S0 vacuum expectation value
S0 background field


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ωk(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ωk(t0)


ΩΛ(t0) the current era
Ω¯M(t)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
ΩM(t0) the current era


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯M(t)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯M(t0)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯M(t)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩΛ(t) negative


ΩΛ(t0) the current era
Ω¯M(t0)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩΛ(t) control


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0) the quantity


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0) the quantity


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩM(t) future


ΩΛ(t0) the current era
Ω¯M(t0)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ω¯Λ(t)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
ΩM(t0) the current era


ΩΛ(t0) the current era
ΩM(t)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
Ω¯Λ(t)


ΩΛ(t0) the current era
Ω¯M(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ω¯Λ(t0)


ΩΛ(t0) the current era
Ω¯M(t0)


ΩΛ(t0) the current era
ΩM(t0)


ΩΛ(t0) the current era
Ωk(t0) orders


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
Ω¯M(t0) era


ΩΛ(t0) the current era
Ω¯Λ(t0) the current era


ΩΛ(t0) the current era
ΩΛ(t)


ΩΛ(t0) the current era
ΩΛ(t)


-g00(r)=1-2β*/r+γ*r
γ0


G constant
Geff small, negative


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff


G constant
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G constant
Geff


G constant
Geff


G constant
Geff


G constant
GF Fermi’s


G constant
Geff


G constant
Geff the cosmological


G constant
Geff a small, negative


G constant
Geff an appropriate


G constant
Geff


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
Ωk(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ωk(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0) the current era


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t) negative


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t) control


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) the current era


Ω¯Λ(t0) the quantity
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩM(t) future


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
Ω¯Λ(t)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) the standard model


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩM(t0) the current era


Ω¯Λ(t0) the quantity
ΩM(t)


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ω¯Λ(t)


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0) it


Ω¯Λ(t0) the quantity
Ω¯M(t0)


Ω¯Λ(t0) the quantity
ΩM(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
Ωk(t0) orders


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
Ω¯M(t0) era


Ω¯Λ(t0) the quantity
ΩΛ(t)


Ω¯Λ(t0) the quantity
ΩΛ(t0)


Ω¯Λ(t0) the quantity
ΩΛ(t)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0 urfeld


α=-2λS02 parameters
S0 field


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0 larger


α=-2λS02 parameters
S0 vacuum expectation value


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0 a large rather than a small


α=-2λS02 parameters
S0 scale parameter


α=-2λS02 parameters
S0 a constant value


α=-2λS02 parameters
αg constant


α=-2λS02 parameters
αg constant


α=-2λS02 parameters
αg


α=-2λS02 parameters
-2λS02


α=-2λS02 parameters
S0 non-zero


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0


α=-2λS02 parameters
S0 background field


q(t)
q(t0)


q(t)
q0


q(t)
q(t0)


q(t)
q(t0)


q(t)
t0 age


q(t)
q0


q(t)
q(t0)


q(t)
q(t0)


q(t)
q(t0)


α the parameter
αg constant


α the parameter
αg constant


α the parameter
αg


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ωk(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ωk(t0)


ΩΛ(t0) the same order of magnitude
Ω¯M(t)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0) the current era


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯M(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯M(t0)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯M(t)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t) negative


ΩΛ(t0) the same order of magnitude
Ω¯M(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩΛ(t) control


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0) the quantity


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0) the quantity


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t) future


ΩΛ(t0) the same order of magnitude
Ω¯M(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
ΩM(t0) the current era


ΩΛ(t0) the same order of magnitude
ΩM(t)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t)


ΩΛ(t0) the same order of magnitude
Ω¯M(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0)


ΩΛ(t0) the same order of magnitude
Ω¯M(t0)


ΩΛ(t0) the same order of magnitude
ΩM(t0)


ΩΛ(t0) the same order of magnitude
Ωk(t0) orders


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
Ω¯M(t0) era


ΩΛ(t0) the same order of magnitude
Ω¯Λ(t0) the current era


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ΩΛ(t0) the same order of magnitude
ΩΛ(t)


ρM(t)>0
ρM(t0)


ρM(t)>0
ρM(t0)


ρM(t)>0
t0 age


ρM(t)>0
ρM(t0)


ρM(t)>0
ρM(t0) order


ρM(t)>0
ρM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ds2=Ω(τ,ρ)[c2dτ2-R2(τ)(dρ2+ρ2dΩ)/(1-ρ2γ02/16)2]
γ0


ds2=Ω(τ,ρ)[c2dτ2-R2(τ)(dρ2+ρ2dΩ)/(1-ρ2γ02/16)2]
dL


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
Ωk(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ωk(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0) the current era


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯M(t)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t) negative


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t) control


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) the current era


0Ω¯Λ(t0)1
ΩΛ(t0) the same order of magnitude


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩM(t) future


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
Ω¯Λ(t)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) the standard model


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩM(t0) the current era


0Ω¯Λ(t0)1
ΩM(t)


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ω¯Λ(t)


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩΛ(t0) it


0Ω¯Λ(t0)1
Ω¯M(t0)


0Ω¯Λ(t0)1
ΩM(t0)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
Ωk(t0) orders


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
Ω¯M(t0) era


0Ω¯Λ(t0)1
0ΩΛ(t)1


0Ω¯Λ(t0)1
ΩΛ(t)


0Ω¯Λ(t0)1
ΩΛ(t0)


0Ω¯Λ(t0)1
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


ΩΛ(t,α=0,k<0)
t0 age


ΩΛ(t,α=0,k<0)
αg constant


ΩΛ(t,α=0,k<0)
αg constant


ΩΛ(t,α=0,k<0)
αg


α<0
αg constant


α<0
αg constant


α<0
αg


Geff
GF Fermi’s


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


α
αg constant


α
αg constant


α
αg


Tkinμν=0
TV a large


Tkinμν=0
Tmax


Tkinμν=0
TV big or small


Tkinμν=0
TV


Tkinμν=0
Tmax


Tkinμν=0
Tmax


Tkinμν=0
TV


Tkinμν=0
Tmax


Tkinμν=0
Tμν


Tkinμν=0
Tmax


Tkinμν=0
TV


Tkinμν=0
Tμν the associated energy-momentum tensor


Tkinμν=0
Tmax


Tkinμν=0
TV


Tkinμν=0
TV (highest) critical temperature


Tkinμν=0
Tmax


Tkinμν=0
Tμν


Tkinμν=0
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tkinμν=0
Tmax


Tkinμν=0
TV


Tkinμν=0
TV


Tkinμν=0
Tμν=0 motion


Tkinμν=0
Tmax


Tkinμν=0
TV


Tkinμν=0
TV


Tkinμν=0
Tmax the temperature


αc2
αg constant


αc2
αg constant


αc2
αg


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


S0
S0


S0
S0


S0
S0 vacuum expectation value


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


α0
αg constant


α0
αg constant


α0
αg


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t) negative


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t) control


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
t0 age


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)=8πGΛ/3cH2(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t) future


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
GF Fermi’s


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) the standard model


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0) it


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩM(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ωk(t0) orders


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯M(t0) era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
Ω¯Λ(t0) the current era


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t0)


Ω¯Λ(t)=8πGeffΛ/3cH2(t)
ΩΛ(t)


c3/16πG
Geff small, negative


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
Geff


c3/16πG
GF Fermi’s


c3/16πG
Geff


c3/16πG
Geff the cosmological


c3/16πG
Geff a small, negative


c3/16πG
Geff an appropriate


c3/16πG
Geff


Geff
GF Fermi’s


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
Ωk(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ωk(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩM(t0) the current era


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ω¯M(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩΛ(t) negative


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
Ω¯M(t0)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t) control


Ω¯M(t)=O(10-60)
t0 age


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0) the quantity


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0) the current era


Ω¯M(t)=O(10-60)
Ω¯Λ(t0) the quantity


Ω¯M(t)=O(10-60)
ΩΛ(t0) the same order of magnitude


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩM(t) future


Ω¯M(t)=O(10-60)
Ω¯M(t0)


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0) the standard model


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
10-2 order


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
ΩM(t0) the current era


Ω¯M(t)=O(10-60)
ΩM(t)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t)


Ω¯M(t)=O(10-60)
Ω¯M(t0)


Ω¯M(t)=O(10-60)
1060 order


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0) it


Ω¯M(t)=O(10-60)
Ω¯Λ(t0)


Ω¯M(t)=O(10-60)
Ω¯M(t0)


Ω¯M(t)=O(10-60)
ΩM(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
Ωk(t0) orders


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
Ω¯M(t0) era


Ω¯M(t)=O(10-60)
Ω¯Λ(t0) the current era


Ω¯M(t)=O(10-60)
ΩΛ(t)


Ω¯M(t)=O(10-60)
ΩΛ(t0)


Ω¯M(t)=O(10-60)
ΩΛ(t)


α
αg constant


α
αg constant


α
αg


R(t)et
t0 age


Ωk(t0)=0
Ω¯M(t0)=0 the rather tight


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ωk(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t) negative


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t) control


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the current era


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩΛ(t0) the same order of magnitude


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t) future


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the standard model


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0 viz.


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0) it


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯M(t0) era


Ωk(t0)=0
Ω¯Λ(t0) the current era


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


-q(t0)H2(t0)=αc2
q0


-q(t0)H2(t0)=αc2
αg constant


-q(t0)H2(t0)=αc2
αg constant


-q(t0)H2(t0)=αc2
q0


-q(t0)H2(t0)=αc2
αg


-q(t0)H2(t0)=αc2
-q(t)H2(t)


ΩΛ(t,α>0) the faster
t0 age


ΩΛ(t,α>0) the faster
αg constant


ΩΛ(t,α>0) the faster
αg constant


ΩΛ(t,α>0) the faster
αg


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ωk(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t) negative


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t) control


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t) future


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0) orders


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯M(t0) era


ΩΛ(t0)=0.7
Ω¯Λ(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


α
αg constant


α
αg constant


α
αg


α=0
αg constant


α=0
αg constant


α=0
αg


H2(t0)=-αc2/q(t0)
q0


H2(t0)=-αc2/q(t0)
αg constant


H2(t0)=-αc2/q(t0)
αg constant


H2(t0)=-αc2/q(t0)
q0


H2(t0)=-αc2/q(t0)
αg


ρM(t0)
ρM(t) perfectly normal


ρM(t0)
ρM(t)


ρM(t0)
ρM(t)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
Ωk(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ωk(t0)


ΩM(t) future
Ω¯M(t)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩM(t0) the current era


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯M(t)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯M(t0)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯M(t)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩΛ(t) negative


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
Ω¯M(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩΛ(t) control


ΩM(t) future
t0 age


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯Λ(t0) the quantity


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩΛ(t0) the current era


ΩM(t) future
Ω¯Λ(t0) the quantity


ΩM(t) future
ΩΛ(t0) the same order of magnitude


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯M(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
Ω¯Λ(t)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩΛ(t0) the standard model


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩM(t0) the current era


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
Ω¯Λ(t)


ΩM(t) future
Ω¯M(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
ΩΛ(t0) it


ΩM(t) future
Ω¯Λ(t0)


ΩM(t) future
Ω¯M(t0)


ΩM(t) future
ΩM(t0)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
Ωk(t0) orders


ΩM(t) future
ΩΛ(t)


ΩM(t) future
Ω¯M(t0) era


ΩM(t) future
Ω¯Λ(t0) the current era


ΩM(t) future
ΩΛ(t)


ΩM(t) future
ΩΛ(t0)


ΩM(t) future
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ωk(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ωk(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t) negative


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t) control


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the current era


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t) future


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the standard model


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0) it


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ωk(t0) orders


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0) the current era


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


S0 a large rather than a small
S0


S0 a large rather than a small
S0


S0 a large rather than a small
S0 vacuum expectation value


T2(t0)Tmax2/TV4 the quantity
TV a large


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
TV big or small


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
Tkinμν


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
Tμν


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
Tμν the associated energy-momentum tensor


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
TV (highest) critical temperature


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
Tμν


T2(t0)Tmax2/TV4 the quantity
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
VminGL which


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
Tmax


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
TV


T2(t0)Tmax2/TV4 the quantity
Tmax the temperature


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV a large


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV big or small


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tkinμν


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tμν


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tμν the associated energy-momentum tensor


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
tanh(α1/2ct0)


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV (highest) critical temperature


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tμν


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
αg constant


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
αg constant


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
αg


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
VminGL which


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
TV


-tanh2(α1/2ct0)=-(1+T2(t0)Tmax2/TV4)-1
Tmax the temperature


ρM(t)
ρM(t0)


ρM(t)
ρM(t0)


ρM(t)
t0 age


ρM(t)
ρM(t0)


ρM(t)
ρM(t0) order


ρM(t)
ρM(t0)


S0 scale parameter
S0


S0 scale parameter
S0


S0 scale parameter
S0 vacuum expectation value


GF Fermi’s
Geff small, negative


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff


GF Fermi’s
Geff the cosmological


GF Fermi’s
Geff a small, negative


GF Fermi’s
Geff an appropriate


GF Fermi’s
Geff


ρM(t)=B/R3(t)
ρM(t0)


ρM(t)=B/R3(t)
ρM(t0)


ρM(t)=B/R3(t)
t0 age


ρM(t)=B/R3(t)
ρM(t0)


ρM(t)=B/R3(t)
ρM(t0) order


ρM(t)=B/R3(t)
ρM(t0)


ΩΛ(t0)=0
Ω¯M(t0)=0 the rather tight


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ωk(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t0) the current era


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯M(t)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t) negative


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩΛ(t) control


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯M(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
ΩM(t) future


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ω¯Λ(t)


ΩΛ(t0)=0
ΩM(t0)=0


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
ΩM(t0)=0


ΩΛ(t0)=0
ΩM(t0) the current era


ΩΛ(t0)=0
ΩM(t)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ω¯M(t0)=0 viz.


ΩΛ(t0)=0
Ω¯Λ(t)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯Λ(t0)


ΩΛ(t0)=0
Ω¯M(t0)


ΩΛ(t0)=0
ΩM(t0)


ΩΛ(t0)=0
Ωk(t0) orders


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
Ωk(t0)=0


ΩΛ(t0)=0
Ω¯M(t0) era


ΩΛ(t0)=0
Ω¯Λ(t0) the current era


ΩΛ(t0)=0
ΩΛ(t)


ΩΛ(t0)=0
ΩΛ(t)


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0 urfeld


Sμμ+SRμμ/6=0 field equation
S0 field


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0 larger


Sμμ+SRμμ/6=0 field equation
S0 vacuum expectation value


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0 a large rather than a small


Sμμ+SRμμ/6=0 field equation
S0 scale parameter


Sμμ+SRμμ/6=0 field equation
S0 a constant value


Sμμ+SRμμ/6=0 field equation
S0 non-zero


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0


Sμμ+SRμμ/6=0 field equation
S0 background field


Tμν
TV a large


Tμν
Tmax


Tμν
TV big or small


Tμν
TV


Tμν
Tmax


Tμν
Tmax


Tμν
Tkinμν


Tμν
TV


Tμν
Tmax


Tμν
Tmax


Tμν
TV


Tμν
Tmax


Tμν
TV


Tμν
TV (highest) critical temperature


Tμν
Tmax


Tμν
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tμν
Tmax


Tμν
TV


Tμν
TV


Tμν
Tmax


Tμν
TV


Tμν
TV


Tμν
Tmax the temperature


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ωk(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ωk(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t0) the current era


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t) negative


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t) control


Ω¯Λ(t)
t0 age


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0) the current era


Ω¯Λ(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t) future


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0) the standard model


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0) the current era


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t0) it


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ωk(t0) orders


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
Ω¯M(t0) era


Ω¯Λ(t)
Ω¯Λ(t0) the current era


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t0)=0 the rather tight


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ωk(t)


ΩM(t0)=0
Ωk(t0)


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
ΩΛ(t0)=0


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t) negative


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t) control


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯Λ(t0) the quantity


ΩM(t0)=0
ΩΛ(t0) the current era


ΩM(t0)=0
Ω¯Λ(t0) the quantity


ΩM(t0)=0
ΩΛ(t0) the same order of magnitude


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
ΩM(t) future


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t0)=0


ΩM(t0)=0
Ω¯Λ(t)


ΩM(t0)=0
ΩΛ(t0) the standard model


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯M(t0)=0 viz.


ΩM(t0)=0
Ω¯Λ(t)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0) it


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ωk(t0) orders


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
Ω¯M(t0) era


ΩM(t0)=0
Ω¯Λ(t0) the current era


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t)


Geff
GF Fermi’s


λS4
S0


λS4
S0


λS4
S0 urfeld


λS4
S0 field


λS4
S0


λS4
S0


λS4
S0 larger


λS4
S0 vacuum expectation value


λS4
S0


λS4
S0 a large rather than a small


λS4
S0 scale parameter


λS4
S0 a constant value


λS4
S0 non-zero


λS4
S0


λS4
S0


λS4
S0 background field


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV a large


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff small, negative


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV big or small


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 urfeld


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 field


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
LPL-1 inverse Planck length


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tkinμν


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tμν


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tμν the associated energy-momentum tensor


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 larger


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV (highest) critical temperature


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 vacuum expectation value


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 a large rather than a small


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 scale parameter


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
GF Fermi’s


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tμν


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
LPL-1


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 a constant value


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff the cosmological


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
VminGL which


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 non-zero


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff a small, negative


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff an appropriate


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
TV


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Geff


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
Tmax the temperature


VGL(S,T)=gS4-2g(TV2-T2)S2 effective Ginzburg-Landau potential
S0 background field


S0 a constant value
S0


S0 a constant value
S0


S0 a constant value
S0 vacuum expectation value


S(x) field
S0


S(x) field
S0


S(x) field
S0 urfeld


S(x) field
S0 field


S(x) field
S0


S(x) field
S0


S(x) field
S0 larger


S(x) field
S0 vacuum expectation value


S(x) field
S0


S(x) field
S0 a large rather than a small


S(x) field
S0 scale parameter


S(x) field
S0 a constant value


S(x) field
S0 non-zero


S(x) field
S0


S(x) field
S0


S(x) field
S0 background field


TmaxT(t0)
TV a large


TmaxT(t0)
TVT(t0)


TmaxT(t0)
TV big or small


TmaxT(t0)
TV


TmaxT(t0)
T(t)


TmaxT(t0)
TVT(t0)


TmaxT(t0)
Tkinμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
Tμν the associated energy-momentum tensor


TmaxT(t0)
TV


TmaxT(t0)
TV (highest) critical temperature


TmaxT(t0)
Tμν


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


TmaxT(t0)
TV


dL=cH(t0)-12(1+z)[1-(1+z)-1/2] the (too bright for the data)
LPL-1 inverse Planck length


dL=cH(t0)-12(1+z)[1-(1+z)-1/2] the (too bright for the data)
LPL-1


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ωk(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ωk(t0)


ΩΛ(t0) the standard model
Ω¯M(t)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
ΩM(t0) the current era


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯M(t)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯M(t0)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯M(t)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩΛ(t) negative


ΩΛ(t0) the standard model
Ω¯M(t0)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩΛ(t) control


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0) the quantity


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0) the quantity


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩM(t) future


ΩΛ(t0) the standard model
Ω¯M(t0)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
ΩM(t0) the current era


ΩΛ(t0) the standard model
ΩM(t)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
Ω¯Λ(t)


ΩΛ(t0) the standard model
Ω¯M(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ω¯Λ(t0)


ΩΛ(t0) the standard model
Ω¯M(t0)


ΩΛ(t0) the standard model
ΩM(t0)


ΩΛ(t0) the standard model
Ωk(t0) orders


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
Ω¯M(t0) era


ΩΛ(t0) the standard model
Ω¯Λ(t0) the current era


ΩΛ(t0) the standard model
ΩΛ(t)


ΩΛ(t0) the standard model
ΩΛ(t)


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV a large


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV big or small


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tkinμν


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tμν


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tμν the associated energy-momentum tensor


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV (highest) critical temperature


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tμν


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
TV


4g00=3(T00-Trr)/4αgg00-f(r) equation
Tmax the temperature


α>0, k<0
αg constant


α>0, k<0
αg constant


α>0, k<0
αg


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


10-2 order
10-60 order


10-2 order
1060 order


T(t0)
TV a large


T(t0)
Tmax


T(t0)
TV big or small


T(t0)
TV


T(t0)
T(t)


T(t0)
Tmax


T(t0)
Tmax


T(t0)
Tkinμν


T(t0)
TV


T(t0)
Tmax


T(t0)
Tμν


T(t0)
Tmax


T(t0)
TV


T(t0)
Tμν the associated energy-momentum tensor


T(t0)
Tmax


T(t0)
TV


T(t0)
TV (highest) critical temperature


T(t0)
Tmax


T(t0)
Tμν


T(t0)
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


T(t0)
Tmax


T(t0)
TV


T(t0)
TV


T(t0)
Tmax


T(t0)
TV


T(t0)
TV


T(t0)
Tmax the temperature


β
β*


G an effective negative cosmological
Geff small, negative


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff


G an effective negative cosmological
GF Fermi’s


G an effective negative cosmological
Geff


G an effective negative cosmological
Geff the cosmological


G an effective negative cosmological
Geff a small, negative


G an effective negative cosmological
Geff an appropriate


G an effective negative cosmological
Geff


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ωk(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0) the current era


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q0


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
t0 age


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0) the quantity


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0) the current era


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0) the quantity


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0) the same order of magnitude


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t) future


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0) the standard model


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
q0


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0) the current era


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0) it


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩM(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ωk(t0) orders


-q(t)=ΩΛ(t)=1-Ωk(t)
q(t0)


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯M(t0) era


-q(t)=ΩΛ(t)=1-Ωk(t)
Ω¯Λ(t0) the current era


-q(t)=ΩΛ(t)=1-Ωk(t)
ΩΛ(t0)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV a large


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV big or small


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
Tkinμν


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
Tμν


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
Tμν the associated energy-momentum tensor


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV (highest) critical temperature


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
Tμν


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time
TV


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


q(t0)=-0.37
q0


q(t0)=-0.37
q(t) conformal cosmology


q(t0)=-0.37
q(t)


q(t0)=-0.37
q0


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
Ωk(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯M(t)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩM(t0) the current era


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯M(t)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯M(t0)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯M(t)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩΛ(t) negative


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
Ω¯M(t0)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩΛ(t) control


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯Λ(t0) the quantity


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩΛ(t0) the current era


Ωk(t0)0
Ω¯Λ(t0) the quantity


Ωk(t0)0
ΩΛ(t0) the same order of magnitude


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩM(t) future


Ωk(t0)0
Ω¯M(t0)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
Ω¯Λ(t)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩΛ(t0) the standard model


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩM(t)


Ωk(t0)0
ΩM(t0) the current era


Ωk(t0)0
ΩM(t)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
Ω¯Λ(t)


Ωk(t0)0
Ω¯M(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
ΩΛ(t0) it


Ωk(t0)0
Ω¯Λ(t0)


Ωk(t0)0
Ω¯M(t0)


Ωk(t0)0
ΩM(t0)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
Ω¯M(t0) era


Ωk(t0)0
Ω¯Λ(t0) the current era


Ωk(t0)0
ΩΛ(t)


Ωk(t0)0
ΩΛ(t0)


Ωk(t0)0
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
Ωk(t)


ΩM(t0)=1
Ωk(t0)


ΩM(t0)=1
Ω¯M(t)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
Ω¯M(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t0)=1


ΩM(t0)=1
Ω¯M(t0)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
Ω¯M(t)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t) negative


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
Ω¯M(t0)


ΩM(t0)=1
ΩΛ(t) control


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
Ω¯Λ(t0) the quantity


ΩM(t0)=1
Ωk(t0)=1


ΩM(t0)=1
Ωk(t0)=1


ΩM(t0)=1
ΩΛ(t0) the current era


ΩM(t0)=1
Ω¯Λ(t0) the quantity


ΩM(t0)=1
ΩΛ(t0) the same order of magnitude


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
ΩM(t) future


ΩM(t0)=1
Ω¯M(t0)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
Ω¯Λ(t)


ΩM(t0)=1
ΩΛ(t0) the standard model


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
ΩM(t)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
Ω¯Λ(t)


ΩM(t0)=1
Ω¯M(t0)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
ΩΛ(t0) it


ΩM(t0)=1
Ω¯Λ(t0)


ΩM(t0)=1
Ω¯M(t0)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
Ωk(t0) orders


ΩM(t0)=1
Ωk(t0)=1


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
Ω¯M(t0) era


ΩM(t0)=1
Ω¯Λ(t0) the current era


ΩM(t0)=1
ΩΛ(t)


ΩM(t0)=1
ΩΛ(t0)


ΩM(t0)=1
ΩΛ(t)


-cΛ=-cλS04=σTV4
TV a large


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
TV big or small


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
S0 urfeld


-cΛ=-cλS04=σTV4
S0 field


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
Tkinμν


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
Tμν


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
Tμν the associated energy-momentum tensor


-cΛ=-cλS04=σTV4
S0 larger


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
TV (highest) critical temperature


-cΛ=-cλS04=σTV4
S0 vacuum expectation value


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
S0 a large rather than a small


-cΛ=-cλS04=σTV4
S0 scale parameter


-cΛ=-cλS04=σTV4
Tμν


-cΛ=-cλS04=σTV4
S0 a constant value


-cΛ=-cλS04=σTV4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
VminGL which


-cΛ=-cλS04=σTV4
S0 non-zero


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
S0


-cΛ=-cλS04=σTV4
Tmax


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
TV


-cΛ=-cλS04=σTV4
Tmax the temperature


-cΛ=-cλS04=σTV4
S0 background field


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


tanh2(3D1/2t/2)
t0 age


Geff the cosmological
GF Fermi’s


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ωk(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ωk(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0) the current era


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t) negative


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t) control


Ω¯Λ(t)/Ω¯M(t)
t0 age


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0) the current era


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t) future


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0) the standard model


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0) the current era


Ω¯Λ(t)/Ω¯M(t)
ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)/ΩM(t)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0) it


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩM(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
Ωk(t0) orders


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
Ω¯M(t0) era


Ω¯Λ(t)/Ω¯M(t)
Ω¯Λ(t0) the current era


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t0)


Ω¯Λ(t)/Ω¯M(t)
ΩΛ(t)


α>0, k>0
αg constant


α>0, k>0
αg constant


α>0, k>0
αg


q(t)-1
q(t0)


q(t)-1
q0


q(t)-1
q(t0)


q(t)-1
q(t0)


q(t)-1
t0 age


q(t)-1
q0


q(t)-1
q(t0)


q(t)-1
q(t0)


q(t)-1
q(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ωk(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯M(t)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t) negative


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩΛ(t) control


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0) the quantity


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t) future


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
ΩM(t0) the current era


ΩΛ(t0)=0.7
ΩM(t)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯Λ(t)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯Λ(t0)


ΩΛ(t0)=0.7
Ω¯M(t0)


ΩΛ(t0)=0.7
ΩM(t0)


ΩΛ(t0)=0.7
Ωk(t0) orders


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
Ω¯M(t0) era


ΩΛ(t0)=0.7
Ω¯Λ(t0) the current era


ΩΛ(t0)=0.7
ΩΛ(t)


ΩΛ(t0)=0.7
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t0)=0 the rather tight


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ωk(t)


ΩM(t0)=0
Ωk(t0)


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
ΩΛ(t0)=0


ΩM(t0)=0
Ω¯M(t)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t) negative


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t) control


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯M(t0)=0


ΩM(t0)=0
Ω¯Λ(t0) the quantity


ΩM(t0)=0
ΩΛ(t0) the current era


ΩM(t0)=0
Ω¯Λ(t0) the quantity


ΩM(t0)=0
ΩΛ(t0) the same order of magnitude


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
ΩM(t) future


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩΛ(t0)=0


ΩM(t0)=0
Ω¯Λ(t)


ΩM(t0)=0
ΩΛ(t0) the standard model


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
ΩM(t)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ω¯M(t0)=0 viz.


ΩM(t0)=0
Ω¯Λ(t)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
ΩΛ(t0) it


ΩM(t0)=0
Ω¯Λ(t0)


ΩM(t0)=0
Ω¯M(t0)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
Ωk(t0) orders


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
Ωk(t0)=0


ΩM(t0)=0
Ω¯M(t0) era


ΩM(t0)=0
Ω¯Λ(t0) the current era


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)=0
ΩΛ(t0)


ΩM(t0)=0
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ωk(t)


ΩM(t0)ΩΛ(t0)
Ωk(t0)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t) negative


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t) control


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩM(t) future


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
ΩM(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0)


ΩM(t0)ΩΛ(t0)
Ωk(t0) orders


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
Ω¯M(t0) era


ΩM(t0)ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩM(t0)ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ωk(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ωk(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t) negative


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t) control


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t) future


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ωk(t0) orders


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯M(t0) era


ΩΛ(t0)=ΩM(t0)+1/2 line
Ω¯Λ(t0) the current era


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2 line
ΩΛ(t)


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0 urfeld


λ=λS04/S04λ
S0 field


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0 larger


λ=λS04/S04λ
S0 vacuum expectation value


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0 a large rather than a small


λ=λS04/S04λ
S0 scale parameter


λ=λS04/S04λ
λS4


λ=λS04/S04λ
S0 a constant value


λ=λS04/S04λ
λS4


λ=λS04/S04λ
S0 non-zero


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0


λ=λS04/S04λ
S0 background field


TV4/T4
TV a large


TV4/T4
Tmax


TV4/T4
TV big or small


TV4/T4
TV


TV4/T4
Tmax/TV such a choice


TV4/T4
Tmax


TV4/T4
Tmax


TV4/T4
T4/TV4


TV4/T4
Tkinμν


TV4/T4
TV


TV4/T4
Tmax


TV4/T4
Tμν


TV4/T4
Tmax


TV4/T4
TV


TV4/T4
Tμν the associated energy-momentum tensor


TV4/T4
Tmax


TV4/T4
TV


TV4/T4
TV (highest) critical temperature


TV4/T4
Tmax


TV4/T4
Tμν


TV4/T4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV4/T4
Tmax


TV4/T4
TV


TV4/T4
VminGL which


TV4/T4
TV


TV4/T4
Tmax


TV4/T4
TV


TV4/T4
TV


TV4/T4
Tmax the temperature


ρM(t0) order
ρM(t) perfectly normal


ρM(t0) order
ρM(t)


ρM(t0) order
ρM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
q(t)=(n/2-1)ΩM(t)-ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ωk(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ωk(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0) the current era


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
q0


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t) negative


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t) control


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0) the quantity


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
q(t) conformal cosmology


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0) the quantity


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
q(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t) future


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
q0


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0) the current era


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩM(t0)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ωk(t0) orders


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯M(t0) era


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
Ω¯Λ(t0) the current era


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


q(t0)=(n/2-1)ΩM(t0)-ΩΛ(t0)
ΩΛ(t)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ωk(t)


ΩM(t0) the current era
Ωk(t0)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t) negative


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t) control


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0) the quantity


ΩM(t0) the current era
ΩΛ(t0) the current era


ΩM(t0) the current era
Ω¯Λ(t0) the quantity


ΩM(t0) the current era
ΩΛ(t0) the same order of magnitude


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩM(t) future


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t)


ΩM(t0) the current era
ΩΛ(t0) the standard model


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
ΩM(t)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ω¯Λ(t)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
ΩΛ(t0) it


ΩM(t0) the current era
Ω¯Λ(t0)


ΩM(t0) the current era
Ω¯M(t0)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
Ωk(t0) orders


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
Ω¯M(t0) era


ΩM(t0) the current era
Ω¯Λ(t0) the current era


ΩM(t0) the current era
ΩΛ(t)


ΩM(t0) the current era
ΩΛ(t0)


ΩM(t0) the current era
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ωk(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ωk(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t) negative


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t) control


ΩM(t)
t0 age


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the current era


ΩM(t)
Ω¯Λ(t0) the quantity


ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0) the standard model


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩM(t0) the current era


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ω¯Λ(t)


ΩM(t)
Ω¯M(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
ΩΛ(t0) it


ΩM(t)
Ω¯Λ(t0)


ΩM(t)
Ω¯M(t0)


ΩM(t)
ΩM(t0)


ΩM(t)
ΩΛ(t0)


ΩM(t)
Ωk(t0) orders


ΩM(t)
ΩΛ(t)


ΩM(t)
Ω¯M(t0) era


ΩM(t)
Ω¯Λ(t0) the current era


ΩM(t)
ΩΛ(t)


ΩM(t)
ΩΛ(t0)


ΩM(t)
ΩΛ(t)


β*=drf(r)r4/12
dL


-2λS02
S0


-2λS02
S0


-2λS02
S0 urfeld


-2λS02
S0 field


-2λS02
S0


-2λS02
S0


-2λS02
S0 larger


-2λS02
S0 vacuum expectation value


-2λS02
S0


-2λS02
S0 a large rather than a small


-2λS02
S0 scale parameter


-2λS02
S0 a constant value


-2λS02
S0 non-zero


-2λS02
S0


-2λS02
S0


-2λS02
S0 background field


R˙(t=0)
t0 age


q(t0)=0
q0


q(t0)=0
q(t) conformal cosmology


q(t0)=0
q(t)


q(t0)=0
q0


R(t)=(B/cΛ)1/3sinh2/3(3D1/2t/2)
t0 age


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


G the standard attractive
Geff small, negative


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
Geff


G the standard attractive
GF Fermi’s


G the standard attractive
Geff


G the standard attractive
Geff the cosmological


G the standard attractive
Geff a small, negative


G the standard attractive
Geff an appropriate


G the standard attractive
Geff


ρM(t0)
ρM(t) perfectly normal


ρM(t0)
ρM(t)


ρM(t0)
ρM(t)


VminGL which
Geff small, negative


VminGL which
Geff


VminGL which
Geff


VminGL which
LPL-1 inverse Planck length


VminGL which
Geff


VminGL which
Geff


VminGL which
Geff


VminGL which
Geff


VminGL which
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


VminGL which
Geff


VminGL which
Geff


VminGL which
Geff


VminGL which
GF Fermi’s


VminGL which
Geff


VminGL which
LPL-1


VminGL which
Geff the cosmological


VminGL which
Geff a small, negative


VminGL which
Geff an appropriate


VminGL which
Geff


-3c3/4πS02
S0


-3c3/4πS02
S0


-3c3/4πS02
S0 urfeld


-3c3/4πS02
S0 field


-3c3/4πS02
S0


-3c3/4πS02
S0


-3c3/4πS02
S0 larger


-3c3/4πS02
S0 vacuum expectation value


-3c3/4πS02
S0


-3c3/4πS02
S0 a large rather than a small


-3c3/4πS02
S0 scale parameter


-3c3/4πS02
S0 a constant value


-3c3/4πS02
S0 non-zero


-3c3/4πS02
S0


-3c3/4πS02
S0


-3c3/4πS02
S0 background field


ΛVminGL effective
Geff small, negative


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
LPL-1 inverse Planck length


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
Geff


ΛVminGL effective
GF Fermi’s


ΛVminGL effective
Geff


ΛVminGL effective
LPL-1


ΛVminGL effective
Geff the cosmological


ΛVminGL effective
Geff a small, negative


ΛVminGL effective
Geff an appropriate


ΛVminGL effective
Geff


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ωk(t)


ΩM(t0)=0.3
Ωk(t0)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t) negative


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t) control


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the current era


ΩM(t0)=0.3
Ω¯Λ(t0) the quantity


ΩM(t0)=0.3
ΩΛ(t0) the same order of magnitude


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t) future


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
ΩΛ(t0) the standard model


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
ΩM(t)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ω¯Λ(t)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
ΩΛ(t0) it


ΩM(t0)=0.3
Ω¯Λ(t0)


ΩM(t0)=0.3
Ω¯M(t0)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
Ωk(t0) orders


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
Ω¯M(t0) era


ΩM(t0)=0.3
Ω¯Λ(t0) the current era


ΩM(t0)=0.3
ΩΛ(t)


ΩM(t0)=0.3
ΩΛ(t0)


ΩM(t0)=0.3
ΩΛ(t)


α>0
αg constant


α>0
αg constant


α>0
αg


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


G the standard
Geff small, negative


G the standard
Geff


G the standard
Geff


G the standard
Geff


G the standard
Geff


G the standard
Geff


G the standard
Geff


G the standard
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G the standard
Geff


G the standard
Geff


G the standard
Geff


G the standard
GF Fermi’s


G the standard
Geff


G the standard
Geff the cosmological


G the standard
Geff a small, negative


G the standard
Geff an appropriate


G the standard
Geff


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


R(t)=(-B/cΛ)1/3cosh2/3(3D1/2t/2)
t0 age


(β-1)/(β+1)=TV4/Tmax4
TV a large


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
TV big or small


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
Tmax/TV such a choice


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
T4/TV4


(β-1)/(β+1)=TV4/Tmax4
Tkinμν


(β-1)/(β+1)=TV4/Tmax4
β*


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
Tμν


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
Tμν the associated energy-momentum tensor


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
TV (highest) critical temperature


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
Tμν


(β-1)/(β+1)=TV4/Tmax4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
TV4/T4


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
VminGL which


(β-1)/(β+1)=TV4/Tmax4
(β-1)/(β+1)=Tmax4/TV4


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
Tmax


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
TV


(β-1)/(β+1)=TV4/Tmax4
Tmax the temperature


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


λS4
S0


λS4
S0


λS4
S0 urfeld


λS4
S0 field


λS4
S0


λS4
S0


λS4
S0 larger


λS4
S0 vacuum expectation value


λS4
S0


λS4
S0 a large rather than a small


λS4
S0 scale parameter


λS4
S0 a constant value


λS4
S0 non-zero


λS4
S0


λS4
S0


λS4
S0 background field


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ωk(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ωk(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0) the current era


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
t0 age


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0) the current era


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)/ΩM(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩM(t) future


ΩΛ(t)/ΩM(t)
Ω¯M(t0)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0) the standard model


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t)/Ω¯M(t)


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
ΩM(t0) the current era


ΩΛ(t)/ΩM(t)
ΩM(t)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t)


ΩΛ(t)/ΩM(t)
Ω¯M(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0) it


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0)


ΩΛ(t)/ΩM(t)
Ω¯M(t0)


ΩΛ(t)/ΩM(t)
ΩM(t0)


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


ΩΛ(t)/ΩM(t)
Ωk(t0) orders


ΩΛ(t)/ΩM(t)
Ω¯M(t0) era


ΩΛ(t)/ΩM(t)
Ω¯Λ(t0) the current era


ΩΛ(t)/ΩM(t)
ΩΛ(t0)


(β-1)/(β+1)=Tmax4/TV4
TV a large


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
TV big or small


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
Tmax/TV such a choice


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
T4/TV4


(β-1)/(β+1)=Tmax4/TV4
Tkinμν


(β-1)/(β+1)=Tmax4/TV4
β*


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
Tμν


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
Tμν the associated energy-momentum tensor


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
TV (highest) critical temperature


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
Tμν


(β-1)/(β+1)=Tmax4/TV4
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
TV4/T4


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
VminGL which


(β-1)/(β+1)=Tmax4/TV4
(β-1)/(β+1)=TV4/Tmax4


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
Tmax


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
TV


(β-1)/(β+1)=Tmax4/TV4
Tmax the temperature


α>0
αg constant


α>0
αg constant


α>0
αg


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
Ωk(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ωk(t0)


Ω¯M(t0)=0 viz.
Ω¯M(t)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩM(t0) the current era


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ω¯M(t)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
Ωk(t0)=0


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0)=0


Ω¯M(t0)=0 viz.
Ω¯M(t)


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩΛ(t) negative


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t) control


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0) the current era


Ω¯M(t0)=0 viz.
Ω¯Λ(t0) the quantity


Ω¯M(t0)=0 viz.
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ωk(t0)=0


Ω¯M(t0)=0 viz.
ΩM(t) future


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩΛ(t0)=0


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t)


Ω¯M(t0)=0 viz.
ΩM(t0)=0


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0) the standard model


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
ΩM(t0)=0


Ω¯M(t0)=0 viz.
ΩM(t0) the current era


Ω¯M(t0)=0 viz.
ΩM(t)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0) it


Ω¯M(t0)=0 viz.
Ω¯Λ(t0)


Ω¯M(t0)=0 viz.
ΩM(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
Ωk(t0) orders


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
Ωk(t0)=0


Ω¯M(t0)=0 viz.
Ω¯Λ(t0) the current era


Ω¯M(t0)=0 viz.
ΩΛ(t)


Ω¯M(t0)=0 viz.
ΩΛ(t0)


Ω¯M(t0)=0 viz.
ΩΛ(t)


S0 non-zero
S0


S0 non-zero
S0


S0 non-zero
S0 vacuum expectation value


R˙(t=0) overwhelmingly large
t0 age


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ωk(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ωk(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t0) the current era


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯M(t)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t) negative


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t) control


Ω¯Λ(t)
t0 age


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0) the current era


Ω¯Λ(t)
Ω¯Λ(t0) the quantity


Ω¯Λ(t)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t) future


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0) the standard model


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
ΩM(t0) the current era


Ω¯Λ(t)
ΩM(t)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
ΩΛ(t0) it


Ω¯Λ(t)
Ω¯Λ(t0)


Ω¯Λ(t)
Ω¯M(t0)


Ω¯Λ(t)
ΩM(t0)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
Ωk(t0) orders


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
Ω¯M(t0) era


Ω¯Λ(t)
Ω¯Λ(t0) the current era


Ω¯Λ(t)
ΩΛ(t)


Ω¯Λ(t)
ΩΛ(t0)


Ω¯Λ(t)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ωk(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ωk(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t) negative


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t) control


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the current era


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t) future


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the standard model


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0) it


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ωk(t0) orders


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0) the current era


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Geff a small, negative
GF Fermi’s


G the effective
Geff small, negative


G the effective
Geff


G the effective
Geff


G the effective
Geff


G the effective
Geff


G the effective
Geff


G the effective
Geff


G the effective
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G the effective
Geff


G the effective
Geff


G the effective
Geff


G the effective
GF Fermi’s


G the effective
Geff


G the effective
Geff the cosmological


G the effective
Geff a small, negative


G the effective
Geff an appropriate


G the effective
Geff


Ω¯M(t=0)
Ω¯Λ(t=0)


Ω¯M(t=0)
t0 age


Ω¯M(t=0)
ΩM(t=0) initial


Ω¯M(t=0)
ΩΛ(t=0) initial


TVTmaxT(t0)
T(t)


TVTmaxT(t0)
Tkinμν


TVTmaxT(t0)
Tμν


TVTmaxT(t0)
Tμν the associated energy-momentum tensor


TVTmaxT(t0)
Tμν


TVTmaxT(t0)
VminGL which


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


β
β*


R(t)
t0 age


R(t)t
t0 age


S0
S0


S0
S0


S0
S0 vacuum expectation value


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


α matter how large
αg constant


α matter how large
αg constant


α matter how large
αg


1060 order
10-60 order


1060 order
10-2 order


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


IW purely gravitational piece
Wμν


IW purely gravitational piece
Wμν


IW purely gravitational piece
Wμν __TABLE_2__


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


-10120
10-60 order


-10120
-1060 order


-10120
10-2 order


-10120
1060 order


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ωk(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ωk(t0)


ΩΛ(t0) it
Ω¯M(t)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
ΩM(t0) the current era


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯M(t)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯M(t0)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯M(t)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩΛ(t) negative


ΩΛ(t0) it
Ω¯M(t0)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩΛ(t) control


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯Λ(t0) the quantity


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯Λ(t0) the quantity


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩM(t) future


ΩΛ(t0) it
Ω¯M(t0)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ω¯Λ(t)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
ΩM(t0) the current era


ΩΛ(t0) it
ΩM(t)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
Ω¯Λ(t)


ΩΛ(t0) it
Ω¯M(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ω¯Λ(t0)


ΩΛ(t0) it
Ω¯M(t0)


ΩΛ(t0) it
ΩM(t0)


ΩΛ(t0) it
Ωk(t0) orders


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
Ω¯M(t0) era


ΩΛ(t0) it
Ω¯Λ(t0) the current era


ΩΛ(t0) it
ΩΛ(t)


ΩΛ(t0) it
ΩΛ(t)


α parameter
αg constant


α parameter
αg constant


α parameter
αg


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ωk(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ωk(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯M(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t) negative


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t) control


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the current era


Ω¯Λ(t0)
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩM(t) future


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0) the standard model


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩM(t0) the current era


Ω¯Λ(t0)
ΩM(t)


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ω¯Λ(t)


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩΛ(t0) it


Ω¯Λ(t0)
Ω¯M(t0)


Ω¯Λ(t0)
ΩM(t0)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
Ωk(t0) orders


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
Ω¯M(t0) era


Ω¯Λ(t0)
ΩΛ(t)


Ω¯Λ(t0)
ΩΛ(t0)


Ω¯Λ(t0)
ΩΛ(t)


ΩΛ(t,α>0,k<0) spatial 3-curvature
t0 age


ΩΛ(t,α>0,k<0) spatial 3-curvature
αg constant


ΩΛ(t,α>0,k<0) spatial 3-curvature
αg constant


ΩΛ(t,α>0,k<0) spatial 3-curvature
αg


ρM(t)
ρM(t0)


ρM(t)
ρM(t0)


ρM(t)
t0 age


ρM(t)
ρM(t0)


ρM(t)
ρM(t0) order


ρM(t)
ρM(t0)


Tμν=0 motion
TV a large


Tμν=0 motion
Tmax


Tμν=0 motion
TV big or small


Tμν=0 motion
TV


Tμν=0 motion
Tmax


Tμν=0 motion
Tmax


Tμν=0 motion
Tkinμν


Tμν=0 motion
TV


Tμν=0 motion
Tmax


Tμν=0 motion
Tmax


Tμν=0 motion
TV


Tμν=0 motion
Tmax


Tμν=0 motion
TV


Tμν=0 motion
TV (highest) critical temperature


Tμν=0 motion
Tkinμν=0


Tμν=0 motion
Tmax


Tμν=0 motion
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


Tμν=0 motion
Tmax


Tμν=0 motion
TV


Tμν=0 motion
TV


Tμν=0 motion
Tmax


Tμν=0 motion
TV


Tμν=0 motion
TV


Tμν=0 motion
Tmax the temperature


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
Ωk(t)


ΩM(t0)0.3 currently preferred standard model
Ωk(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t) negative


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t) control


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0) the quantity


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0) the current era


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0) the quantity


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0) the same order of magnitude


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
ΩM(t) future


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0) the standard model


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
ΩM(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0) it


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
Ωk(t0) orders


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
Ω¯M(t0) era


ΩM(t0)0.3 currently preferred standard model
Ω¯Λ(t0) the current era


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t0)


ΩM(t0)0.3 currently preferred standard model
ΩΛ(t)


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ωk(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ωk(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯M(t)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t) negative


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t) control


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the current era


Ω¯M(t0)
Ω¯Λ(t0) the quantity


Ω¯M(t0)
ΩΛ(t0) the same order of magnitude


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩM(t) future


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0) the standard model


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
ΩM(t0) the current era


Ω¯M(t0)
ΩM(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ω¯Λ(t)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩΛ(t0) it


Ω¯M(t0)
Ω¯Λ(t0)


Ω¯M(t0)
ΩM(t0)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
Ωk(t0) orders


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
Ω¯Λ(t0) the current era


Ω¯M(t0)
ΩΛ(t)


Ω¯M(t0)
ΩΛ(t0)


Ω¯M(t0)
ΩΛ(t)


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0 urfeld


Λ=λS04 a large rather than a small
S0 field


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0 larger


Λ=λS04 a large rather than a small
S0 vacuum expectation value


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0 a large rather than a small


Λ=λS04 a large rather than a small
S0 scale parameter


Λ=λS04 a large rather than a small
S0 a constant value


Λ=λS04 a large rather than a small
S0 non-zero


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0


Λ=λS04 a large rather than a small
S0 background field


q(t0)=(n/2-1)(1+kc2/R˙2(t0))-nΩ¯Λ(t0)/2)
q0


q(t0)=(n/2-1)(1+kc2/R˙2(t0))-nΩ¯Λ(t0)/2)
q0


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


S0
S0


S0
S0


S0
S0 vacuum expectation value


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ωk(t)


ΩM(t0)
Ωk(t0)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t) negative


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t) control


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the current era


ΩM(t0)
Ω¯Λ(t0) the quantity


ΩM(t0)
ΩΛ(t0) the same order of magnitude


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t) future


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
ΩΛ(t0) the standard model


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩM(t)


ΩM(t0)
ΩM(t)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ω¯Λ(t)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
ΩΛ(t0) it


ΩM(t0)
Ω¯Λ(t0)


ΩM(t0)
Ω¯M(t0)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
Ωk(t0) orders


ΩM(t0)
ΩΛ(t)


ΩM(t0)
Ω¯M(t0) era


ΩM(t0)
Ω¯Λ(t0) the current era


ΩM(t0)
ΩΛ(t)


ΩM(t0)
ΩΛ(t0)


ΩM(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


Geff an appropriate
GF Fermi’s


Tmax
TV a large


Tmax
TV big or small


Tmax
TV


Tmax
Tkinμν


Tmax
TV


Tmax
Tμν


Tmax
TV


Tmax
Tμν the associated energy-momentum tensor


Tmax
TV


Tmax
TV (highest) critical temperature


Tmax
Tμν


Tmax
TV


Tmax
TV


Tmax
TV


Tmax
TV


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
Ωk(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯M(t)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩM(t0) the current era


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯M(t)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯M(t0)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯M(t)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩΛ(t) negative


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
Ω¯M(t0)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩΛ(t) control


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯Λ(t0) the quantity


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩΛ(t0) the current era


Ωk(t0) orders
Ω¯Λ(t0) the quantity


Ωk(t0) orders
ΩΛ(t0) the same order of magnitude


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩM(t) future


Ωk(t0) orders
Ω¯M(t0)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
Ω¯Λ(t)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩΛ(t0) the standard model


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
ΩM(t0) the current era


Ωk(t0) orders
ΩM(t)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
Ω¯Λ(t)


Ωk(t0) orders
Ω¯M(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
ΩΛ(t0) it


Ωk(t0) orders
Ω¯Λ(t0)


Ωk(t0) orders
Ω¯M(t0)


Ωk(t0) orders
ΩM(t0)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
Ω¯M(t0) era


Ωk(t0) orders
Ω¯Λ(t0) the current era


Ωk(t0) orders
ΩΛ(t)


Ωk(t0) orders
ΩΛ(t0)


Ωk(t0) orders
ΩΛ(t)


ΩΛ(t,α>0)
t0 age


ΩΛ(t,α>0)
αg constant


ΩΛ(t,α>0)
αg constant


ΩΛ(t,α>0)
αg


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ωk(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)=1


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯M(t)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t) negative


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t) control


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the current era


Ωk(t0)=1
Ω¯Λ(t0) the quantity


Ωk(t0)=1
ΩΛ(t0) the same order of magnitude


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩM(t) future


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0) the standard model


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0)=1


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
ΩM(t0) the current era


Ωk(t0)=1
ΩM(t)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
Ω¯Λ(t)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
ΩΛ(t0) it


Ωk(t0)=1
Ω¯Λ(t0)


Ωk(t0)=1
Ω¯M(t0)


Ωk(t0)=1
ΩM(t0)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
Ω¯M(t0) era


Ωk(t0)=1
Ω¯Λ(t0) the current era


Ωk(t0)=1
ΩΛ(t)


Ωk(t0)=1
ΩΛ(t0)


Ωk(t0)=1
ΩΛ(t)


q(t0)
q0


q(t0)
q(t) conformal cosmology


q(t0)
q(t)


q(t0)
q0


q(k=0,t0)=1/2
q0


q(k=0,t0)=1/2
q0


ΩM(t=0) initial
Ω¯M(t=0) universe


ΩM(t=0) initial
Ω¯Λ(t=0)


ΩM(t=0) initial
t0 age


ΩM(t=0) initial
Ω¯M(t=0)


ΩM(t=0) initial
ΩΛ(t=0) initial


α<0
αg constant


α<0
αg constant


α<0
αg


TV
Tmax


TV
Tmax


TV
Tmax


TV
Tkinμν


TV
Tmax


TV
Tμν


TV
Tmax


TV
Tμν the associated energy-momentum tensor


TV
Tmax


TV
Tmax


TV
Tμν


TV
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


TV
Tmax


TV
VminGL which


TV
Tmax


TV
Tmax the temperature


Geff
GF Fermi’s


Ω¯Λ(t)H2(t) The quantity
t0 age


Tmax the temperature
TV a large


Tmax the temperature
TV big or small


Tmax the temperature
TV


Tmax the temperature
Tkinμν


Tmax the temperature
TV


Tmax the temperature
Tμν


Tmax the temperature
TV


Tmax the temperature
Tμν the associated energy-momentum tensor


Tmax the temperature
TV


Tmax the temperature
TV (highest) critical temperature


Tmax the temperature
Tμν


Tmax the temperature
TV


Tmax the temperature
TV


Tmax the temperature
TV


Tmax the temperature
TV


ΩM(t=0)+ΩΛ(t=0)=1
t0 age


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0 the rather tight


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ωk(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
Ω¯M(t)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t) negative


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t) control


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯M(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the current era


Ωk(t0)=0
Ω¯Λ(t0) the quantity


Ωk(t0)=0
ΩΛ(t0) the same order of magnitude


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩM(t) future


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩΛ(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0) the standard model


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
ΩM(t0)=0


Ωk(t0)=0
ΩM(t0) the current era


Ωk(t0)=0
ΩM(t)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
Ω¯M(t0)=0 viz.


Ωk(t0)=0
Ω¯Λ(t)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
ΩΛ(t0) it


Ωk(t0)=0
Ω¯Λ(t0)


Ωk(t0)=0
Ω¯M(t0)


Ωk(t0)=0
ΩM(t0)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
Ω¯M(t0) era


Ωk(t0)=0
Ω¯Λ(t0) the current era


Ωk(t0)=0
ΩΛ(t)


Ωk(t0)=0
ΩΛ(t0)


Ωk(t0)=0
ΩΛ(t)


3.06×10-30
10-60 order


3.06×10-30
10-2 order


3.06×10-30
1060 order


S0 background field
S0


S0 background field
S0


S0 background field
S0 vacuum expectation value


ds2=(1+γ0r)c2dt2-dr2/(1+γ0r)-r2dΩ metric
t0 age


ds2=(1+γ0r)c2dt2-dr2/(1+γ0r)-r2dΩ metric
dL


G
Geff small, negative


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff


G
Geff the very structure desired above of an effective cosmological which is to indeed solve the cosmological constant problem


G
Geff


G
Geff


G
Geff


G
GF Fermi’s


G
Geff


G
Geff the cosmological


G
Geff a small, negative


G
Geff an appropriate


G
Geff


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
Ωk(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ωk(t0)


Ω¯M(t0) era
Ω¯M(t)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩM(t0) the current era


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯M(t)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯M(t)


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩΛ(t) negative


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t) control


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯Λ(t0) the quantity


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t0) the current era


Ω¯M(t0) era
Ω¯Λ(t0) the quantity


Ω¯M(t0) era
ΩΛ(t0) the same order of magnitude


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩM(t) future


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
Ω¯Λ(t)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t0) the standard model


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
ΩM(t0) the current era


Ω¯M(t0) era
ΩM(t)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
Ω¯Λ(t)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩΛ(t0) it


Ω¯M(t0) era
Ω¯Λ(t0)


Ω¯M(t0) era
ΩM(t0)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
Ωk(t0) orders


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
Ω¯Λ(t0) the current era


Ω¯M(t0) era
ΩΛ(t)


Ω¯M(t0) era
ΩΛ(t0)


Ω¯M(t0) era
ΩΛ(t)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
Ωk(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ωk(t0)


0ΩΛ(t)1
Ω¯M(t)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩM(t0) the current era


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯M(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯M(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯M(t)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
Ω¯M(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
t0 age


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
0Ω¯Λ(t0)1


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯Λ(t0) the quantity


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩΛ(t0) the current era


0ΩΛ(t)1
Ω¯Λ(t0) the quantity


0ΩΛ(t)1
ΩΛ(t0) the same order of magnitude


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
0Ω¯Λ(t0)1


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩM(t) future


0ΩΛ(t)1
Ω¯M(t0)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
Ω¯Λ(t)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩΛ(t0) the standard model


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
ΩM(t0) the current era


0ΩΛ(t)1
ΩM(t)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
Ω¯Λ(t)


0ΩΛ(t)1
Ω¯M(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
ΩΛ(t0) it


0ΩΛ(t)1
Ω¯Λ(t0)


0ΩΛ(t)1
Ω¯M(t0)


0ΩΛ(t)1
ΩM(t0)


0ΩΛ(t)1
ΩΛ(t0)


0ΩΛ(t)1
Ωk(t0) orders


0ΩΛ(t)1
Ω¯M(t0) era


0ΩΛ(t)1
Ω¯Λ(t0) the current era


0ΩΛ(t)1
ΩΛ(t0)


q(t0)=-1/2
q0


q(t0)=-1/2
q(t) conformal cosmology


q(t0)=-1/2
q(t)


q(t0)=-1/2
q0


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
Ωk(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
Ωk(t0)


Ω¯Λ(t0) the current era
Ω¯M(t)


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t0) the current era


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
Ω¯M(t)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
Ω¯M(t0)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
Ω¯M(t)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩΛ(t) negative


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
Ω¯M(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩΛ(t) control


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩΛ(t0) the current era


Ω¯Λ(t0) the current era
ΩΛ(t0) the same order of magnitude


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩM(t) future


Ω¯Λ(t0) the current era
Ω¯M(t0)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
Ω¯Λ(t)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩΛ(t0) the standard model


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩM(t0) the current era


Ω¯Λ(t0) the current era
ΩM(t)


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
Ω¯Λ(t)


Ω¯Λ(t0) the current era
Ω¯M(t0)


Ω¯Λ(t0) the current era
ΩΛ(t0) it


Ω¯Λ(t0) the current era
Ω¯M(t0)


Ω¯Λ(t0) the current era
ΩM(t0)


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
Ωk(t0) orders


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
Ω¯M(t0) era


Ω¯Λ(t0) the current era
ΩΛ(t)


Ω¯Λ(t0) the current era
ΩΛ(t0)


Ω¯Λ(t0) the current era
ΩΛ(t)


(1+T2Tmax2/TV4)-1 the quantity
TV a large


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
TV big or small


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
Tkinμν


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
Tμν


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
Tμν the associated energy-momentum tensor


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
TV (highest) critical temperature


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
Tμν


(1+T2Tmax2/TV4)-1 the quantity
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
VminGL which


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
Tmax


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
TV


(1+T2Tmax2/TV4)-1 the quantity
Tmax the temperature


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ωk(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ωk(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0) the current era


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
t0 age


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0) the quantity


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0) the current era


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0) the quantity


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0) the same order of magnitude


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t) future


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0) the standard model


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0) the current era


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0) it


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩM(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ωk(t0) orders


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯M(t0) era


ΩΛ(t)=tanh2(3D1/2t/2) dependence
Ω¯Λ(t0) the current era


ΩΛ(t)=tanh2(3D1/2t/2) dependence
ΩΛ(t0)


-q(t)H2(t)
q0


-q(t)H2(t)
t0 age


-q(t)H2(t)
q0


ΩΛ(t,α>0,k<0)
t0 age


ΩΛ(t,α>0,k<0)
αg constant


ΩΛ(t,α>0,k<0)
αg constant


ΩΛ(t,α>0,k<0)
αg


ΩΛ(t=0) initial
Ω¯M(t=0) universe


ΩΛ(t=0) initial
Ω¯Λ(t=0)


ΩΛ(t=0) initial
t0 age


ΩΛ(t=0) initial
Ω¯M(t=0)


ΩΛ(t=0) initial
ΩM(t=0) initial


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ωk(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯M(t)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t) negative


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩΛ(t) control


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0) the quantity


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t) future


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
ΩM(t0) the current era


ΩΛ(t0)
ΩM(t)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯Λ(t)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯Λ(t0)


ΩΛ(t0)
Ω¯M(t0)


ΩΛ(t0)
ΩM(t0)


ΩΛ(t0)
Ωk(t0) orders


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
Ω¯M(t0) era


ΩΛ(t0)
Ω¯Λ(t0) the current era


ΩΛ(t0)
ΩΛ(t)


ΩΛ(t0)
ΩΛ(t)


q(t)=[1-Tmax2/T2(t)]-1 (18
TV a large


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
TV big or small


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax/TV such a choice


q(t)=[1-Tmax2/T2(t)]-1 (18
q0


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
T4/TV4


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
Tkinμν


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
Tμν


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
Tμν the associated energy-momentum tensor


q(t)=[1-Tmax2/T2(t)]-1 (18
t0 age


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
TV (highest) critical temperature


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
Tμν


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax __TABLE_0__ with all the permanently expanding ones thus necessarily being way below their maximum temperatures once given enough time


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
q0


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
TV4/T4


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
q(t0)


q(t)=[1-Tmax2/T2(t)]-1 (18
TV


q(t)=[1-Tmax2/T2(t)]-1 (18
Tmax the temperature


dL
LPL-1 inverse Planck length


dL
LPL-1


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ωk(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ωk(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯M(t)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
t0 age


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the current era


ΩΛ(t)
Ω¯Λ(t0) the quantity


ΩΛ(t)
ΩΛ(t0) the same order of magnitude


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩM(t) future


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0) the standard model


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩM(t)


ΩΛ(t)
ΩM(t0) the current era


ΩΛ(t)
ΩM(t)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ω¯Λ(t)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
ΩΛ(t0) it


ΩΛ(t)
Ω¯Λ(t0)


ΩΛ(t)
Ω¯M(t0)


ΩΛ(t)
ΩM(t0)


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t)
Ωk(t0) orders


ΩΛ(t)
Ω¯M(t0) era


ΩΛ(t)
Ω¯Λ(t0) the current era


ΩΛ(t)
ΩΛ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ωk(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ωk(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t) negative


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t) control


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0) the quantity


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t) future


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩM(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0)


ΩΛ(t0)=ΩM(t0)+1/2
Ωk(t0) orders


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯M(t0) era


ΩΛ(t0)=ΩM(t0)+1/2
Ω¯Λ(t0) the current era


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ΩΛ(t0)=ΩM(t0)+1/2
ΩΛ(t)


ρM(t)=A/R4
ρM(t0)


ρM(t)=A/R4
ρM(t0)


ρM(t)=A/R4
t0 age


ρM(t)=A/R4
ρM(t0)


ρM(t)=A/R4
ρM(t0) order


ρM(t)=A/R4
ρM(t0)